Chapter 7 Modifications
Ben Marwick
In this template book, I have made some modifications inspired by Matthew Salganik’s Open Review Toolkit. The ORT is an excellent project to enable low-friction engagement between the author and readers. However, it pre-dates bookdown and lacks some of its flexibility, so this is an effort to bring some of the features of the ORT into bookdown. I’ve made three modifications: an open review block, a call-to-action block, and added google analytics.
7.0.1 Open review block
This is a custom block that is appearing at the top of each page informing the reader that they can give immediate feedback directly on the page. The HTML for this block is in open_review_block.html
The feedback tool is hypothes.is, which enables sentence-level annotation directly on the page. There is a script in hypothesis.html
, which we call in _output.yml
like this:
bookdown::gitbook:
includes:
in_header: [hypothesis.html, google_analytics.html]
before_body: open_review_block.html
after_body: call_to_action_block.html
css: style.css
The hypothesis.html
file contains a short script that activates the tool on this site. It also enables us to use the icons in the block above. The ORT also had code to track the use of hypothes.is, but I don’t understand how that works, so I haven’t done it here.
There are also additions to style.css
to add a little styling to one of the inline images in the custom block (named rmdreview
), and adds the speech bubbles on the left side of the block:
.h-icon-chevron-left {
background: white;
padding: 3px;
border: #eee 1px solid;
color: #666;
}
.fa-rotate-315 {
-webkit-transform: rotate(315deg);
-moz-transform: rotate(315deg);
-ms-transform: rotate(315deg);
-o-transform: rotate(315deg);
transform: rotate(315deg);
}
.rmdreview {
padding: 1em 1em 1em 5em;
margin-bottom: 0px;
background: #f5f5f5 5px center/3em no-repeat;
position:relative;
}
.rmdreview:before {
content: "\f0e6";
font-family: FontAwesome;
left:10px;
position:absolute;
top:10px;
bottom: 0px;
font-size: 60px;
}
7.0.2 Call-to-action block
The call-to-action block appears at the bottom of each page to invite the reader to submit their email address to receive updates on the book. This enables us to collect email addresses into a google sheet. The custom block looks like this:
This custom block is called rmdsale
, the html for it is stored in all_to_action_block.html
, which we refer to in the _output.yml
file, as above.
The call-to-action block is styled with some css:
.rmdsale {
padding: 1em 1em 1em 4em;
margin-bottom: 0px;
background: #f5f5f5 5px center/3em no-repeat;
position:relative;
}
.rmdsale:before {
content: "\f07a";
font-family: FontAwesome;
left:10px;
position:absolute;
top:15px;
bottom: 0px;
font-size: 40px;
}
The text field for readers to enter their email address is created by code in email_submit.html
, which inserts some elements from a google form into the page.
To make this work, we have to create a new google form (using the ‘old google forms,’ not the current version), and copy over the key and HTML element details from the default form view. Chrome’s element inspector is very handy for identifying the element details that need to go in email_submit.html
.
The confirmation page that the reader sees after they submit their email is not yet elegant, it’s just the default google forms page. I’m not sure what to do about that.
The email addresses collected by this block are visible in my google sheet https://docs.google.com/spreadsheets/d/17Iyr_U-2AnrOVZBRVMhxihD8Ndpw_Pa2vdmCcFzKuPo/edit#gid=688456476
7.0.3 Google analytics
This is already used in many bookdown projects, and is easy to enable. We go to https://analytics.google.com, create a new account, and get the code snippet and paste it into google_analytics.html
. After that, we add a reference to google_analytics.html
in _output.yml
, as noted above. And that’s it for setting up the analytics.
7.0.4 Not yet implemented
Matt’s ORT contains several other features that are not implemented here. These include tracking of hypothes.is use, A/B testing, a tool to translate the book into numerous languages. I’m not sure how to implement those, and would welcome assistance!
7.0.5 Issues
It is important to keep style.css
and the custom html files in the top level directory of the book. I tried putting them all in a directory together, but couldn’t get it to work.
7.0.6 Reuse
The code for the Open Review Toolkit has an MIT license, and so is freely available for reuse. Because this implementation includes some code from that project, the license is used here also:
MIT License
Copyright (c) 2016 Open Review Toolkit & Ben Marwick
Permission is hereby granted, free of charge, to any person obtaining a copy
of this software and associated documentation files (the "Software"), to deal
in the Software without restriction, including without limitation the rights
to use, copy, modify, merge, publish, distribute, sublicense, and/or sell
copies of the Software, and to permit persons to whom the Software is
furnished to do so, subject to the following conditions:
The above copyright notice and this permission notice shall be included in all
copies or substantial portions of the Software.
 IN NO EVENT SHALL THE
AUTHORS OR COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER
LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING FROM,
OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER DEALINGS IN THE
SOFTWARE.
The text of this chapter is licensed under a Creative Commons Attribution 4.0 International License. This means it may be freely reused if appropriate credit is given.


Your title here
Your name here
Markdown Test
###Why Someone can be called Foundation？
* Rich
* Well-equipped with device like girlfriends
* Born with Foundation
中文字体测试
GitHub
Markdown Test
* Hello
* I love you
*I love to be there for you...*
沉思·航
百度
Hello, world
public class Test{
public static void main(String[] args){
System.out.println("Hello, world"); //end up here
}
}
File.read "a.txt" do |file|
file.each_line do |line|
puts line
end
end
<hmtl>
<title>Test</title>

Test Page


Wine Quality
Model Accuracy 82%
Wine Type
Select Type
White Wine
Red Wine
Fixed Acidity
Volatile Acidity
Citric Acid
Residual Sugar
Chlorides
Free Sulfur Dioxide
Total Sulfur Dioxide
Density
PH
Sulphates
Alcohol


These release notes cover new developer and user-facing incompatibilities, important issues, features, and major improvements.
HBASE-9745 | Major | Append HBASE_CLASSPATH to end of Java classpath and use another env var for prefix
The additional JAR files specified with HBASE_CLASSPATH_PREFIX are prefixed to the system JARs.
Committed to 0.96 and trunk. Thanks for the review Elliott.
Tool to check cluster. See $ ./bin/hbase org.apache.hadoop.hbase.tool.RegionServerCanary -help for how to use.
{code} Usage: bin/hbase org.apache.hadoop.hbase.tool.Canary [opts] [table/regionserver 1 [table/regionserver 2...]] where [opts] are: -help Show this help and exit. -regionserver replace the table argument to regionserver, which means to enable regionserver mode -daemon Continuous check at defined intervals. -interval <N> Interval between checks (sec) -e Use region/regionserver as regular expression which means the region/regionserver is regular expression pattern -f <B> stop whole program if first error occurs, default is true -t <N> timeout for a check, default is 600000 (milisecs) {code}
Canary now has different return codes for different types of failures.
Committed this. Thanks Nick for looking.
To import 0.94 exported file in 0.96 cluster or onwards, you need to set system property "hbase.import.version" when running the import command as below:
./bin/hbase -Dhbase.import.version=0.94 org.apache.hadoop.hbase.mapreduce.Import <table name> <import file folder>
Support auto redirect for IE/firefox browsers upon completion of Split/compact operation
Clock skew detection to be made absolute value comparison. Any time difference between master or region, high or low must prevent the region server startup
patch for 0.94.x
The patch makes sure that data block encoding in cache is always the same as that on disk. It deprecates the column family attribute ENCODE_ON_DISK since it doesn't apply any more. HColumnDescriptor#setEncodeOnDisk(boolean) is still there for compatibility issue. However, it doesn't do anything now. HColumnDescriptor#getDataBlockEncodingOnDisk() is also deprecated because the data block encoding on disk is always the same as that in cache for a given store file.
Online encoding change is enabled by default in both trunk and 0.96 now.
Introduces the method TableMapReduceUtil#addHBaseDependencyJars for adding HBase and its direct dependencies (only) to the job configuration.
This is intended as a low-level API, facilitating code reuse between this class and its mapred counterpart. It is also of use to external tools that need to build a MapReduce job that interacts with HBase but want fine-grained control over the jars shipped to the cluster. See also PIG-3285 and HIVE-2055.
Clients now bind to multicast address configured as "hbase.status.multicast.bind.address.ip", <IP_ADDRESS> by default.
$ ./bin/hbase mapredcp --help Usage: hbase mapredcp [-Dtmpjars=...] Construct a CLASSPATH containing dependency jars required to run a mapreduce job. By default, includes any jars detected by TableMapReduceUtils. Provide additional entries by specifying a comma-separated list in tmpjars.
Adds new trace 'start', trace 'status', and trace 'stop' commands to shell.
try run hadoopqa for trunk
WARNING: No release note provided for this change.
New coprocessor to help analysing the performances of the cluster. This coprocessor drops all the writes on the server side, allowing the measure the client and network performances without any limitation on the disk i/o. For a table created like this: create 'usertable', {NAME => 'f1', VERSIONS => 1} . You can then add the coprocessor with this command: alter 'usertable', 'coprocessor' => '|org.apache.hadoop.hbase.tool.WriteSinkCoprocessor|'
Committed 0.96 and trunk. Thanks for reviews.
WARNING: No release note provided for this change.
Forward port of a 0.89fb patch where we issue sync on WAL file construction to force immediate setup of write pipeline (and do it outside of locks so don't hold up writes during setup).


Front End Development Part 1
Media queries let you adapt your site or app depending on the presence or value of various device characteristics and parameters.
In HTML, media queries can be applied to various elements:
link
element's media attribute, they define the media to which a linked resource (typically CSS) should be applied.source
element's media attribute, they define the media to which that source should be applied. (This is only valid inside picture
elements.)style
element's media attribute, they define the media to which the style should be applied.The logical operators not, and, and only can be used to compose a complex media query. You can also combine multiple media queries into a single rule by separating them with commas.
The and operator is used for combining multiple media features together into a single media query, requiring each chained feature to return true in order for the query to be true. It is also used for joining media features with media types.
The not operator is used to negate a media query, returning true if the query would otherwise return false. If present in a comma-separated list of queries, it will only negate the specific query to which it is applied. If you use the not operator, you must also specify a media type.
The only operator is used to apply a style only if an entire query matches, and is useful for preventing older browsers from applying selected styles. If you use the only operator, you must also specify a media type.
Commas are used to combine multiple media queries into a single rule. Each query in a comma-separated list is treated separately from the others. Thus, if any of the queries in a list is true, the entire media statement returns true. In other words, lists behave like a logical or operator.


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|
CBOE Emulator
1.0
|
Logic for maintaining a continuous double auction via a limit-order book. More...
Classes | |
| struct | Limit |
| A price limit containing a FIFO queue of Order objects. More... | |
| class | LimitOrderBook |
| An order book for managing Limit / Order objects in a continuous double auction. More... | |
| struct | LimitTree |
| A single side (buy/sell) of the LimitOrderBook. More... | |
| struct | Order |
| A single order in the LimitOrderBook. More... | |
Typedefs | |
| typedef std::unordered_map< UID, Order > | UIDOrderMap |
| a map of order IDs to orders | |
| typedef tsl::robin_map< Price, Limit * > | PriceLimitMap |
| a map of prices to limit pointers | |
| typedef uint64_t | UID |
| a type for order IDs | |
| typedef uint32_t | Quantity |
| a type for order quantities | |
| typedef uint64_t | Price |
| a type for order prices | |
| typedef uint32_t | Count |
| a type for limit price order counts | |
| typedef uint64_t | Volume |
| a type for limit total volume | |
Enumerations | |
| enum | Side : bool { Sell = false, Buy = true } |
| the possible sides for the LimitTree | |
Functions | |
| template<Side side> | |
| void | set_best (Limit **best, Limit *limit) |
| Set the best to the given limit if the given limit is better. More... | |
| template<> | |
| void | set_best< Side::Buy > (Limit **highest_buy, Limit *limit) |
| Set the best buy to the given limit if the given limit is better. More... | |
| template<> | |
| void | set_best< Side::Sell > (Limit **lowest_sell, Limit *limit) |
| Set the best sell to the given limit if the given limit is better. More... | |
| template<Side side> | |
| void | find_best (Limit **best) |
| Find the next best when removing the best from the tree. More... | |
| template<> | |
| void | find_best< Side::Buy > (Limit **highest_buy) |
| Find the next buy when removing the best buy from the tree. More... | |
| template<> | |
| void | find_best< Side::Sell > (Limit **lowest_sell) |
| Find the next sell when removing the best sell from the tree. More... | |
| template<Side side> | |
| bool | can_match (Price limit, Price market) |
| Return true if the market price can match with the limit price. More... | |
| template<> | |
| bool | can_match< Side::Buy > (Price limit, Price market) |
| Return true if the sell market price can match with the buy limit price. More... | |
| template<> | |
| bool | can_match< Side::Sell > (Price limit, Price market) |
| Return true if the buy market price can match with the sell limit price. More... | |
| Side | operator! (Side side) |
| Return the opposite side using the invert operator. More... | |
Logic for maintaining a continuous double auction via a limit-order book.
Return true if the market price can match with the limit price.
| side | the side of the book to perform the calculation from |
| limit | the price of the limit order (i.e., the best price) |
| market | the price of the opposing side market order to compare |
|
inline |
Return true if the sell market price can match with the buy limit price.
| limit | the price of the buy limit order (i.e., the best price) |
| market | the price of the sell side market order to compare |
|
inline |
Return true if the buy market price can match with the sell limit price.
| limit | the price of the sell limit order (i.e., the best price) |
| market | the price of the buy side market order to compare |
| void DataFeed::LOB::find_best | ( | Limit ** | best | ) |
Find the next best when removing the best from the tree.
| side | the side of the book to perform the calculation from |
| best | the best limit node |
|
inline |
Find the next buy when removing the best buy from the tree.
| highest_buy | the best buy limit node |
|
inline |
Find the next sell when removing the best sell from the tree.
| lowest_sell | the best sell limit node |
Return the opposite side using the invert operator.
| side | the side to invert |
Set the best to the given limit if the given limit is better.
| side | the side of the book to perform the calculation from |
| best | the current best limit |
| limit | the limit node to compare to |
|
inline |
Set the best buy to the given limit if the given limit is better.
| highest_buy | the current best buy limit |
| limit | the buy limit node to compare to |
|
inline |
Set the best sell to the given limit if the given limit is better.
| lowest_sell | the current best sell limit |
| limit | the sell limit node to compare to |


Irelands Traditional Card Game Online
Find Out MoreTwenty-Five could be considered the national card game of Ireland: it is played widely in rural pubs and at home. The game moves quite quickly - it does not take long to play a hand - and although there is a fair amount of luck in it, there is also some scope for skill. It is normally played by about five people but can be played by as few as two or as many as ten. The ranking order of the cards may seem a little arcane at first, but with a little practice it becomes second nature.
Play Now!Twenty-Five Online is a free to play version of the traditional card game. It has been developed using TypeScript to provide card logic and and JavaScript to implement the game rules. The Webapp and game are ran on a NodeJS server. The card graphics are managed by Phaser.io. This is a currently a work in progress and everything is suspect to change. Singleplayer is the only mode available to test currently and not all Singleplayer features are currently implemented.
Contact us with any feedback, suggestions or problems!
123-456-6789


This website was built by Stephen Washington and Reagan Henke. You can find more of Reagan's projects on her Instagram.
The ghost icons were made by Reagan. The "not found" image is from undraw.co. Code for the website is available under the Apache-2.0 License on Github.
Costume images belong to their original copyright holders and are displayed under the fair use provision of copyright law.


THE ICE STORM (Fox Searchlight) Starring: Kevin Kline, Joan Allen, Christina Ricci, Sigourney Weaver, Elijah Wood, Adam Hann-Byrd, Toby Maguire. Screenplay: James Schamus, based on the novel by Rick Moody. Producers: Ted Hope, James Schamus and Ang Lee. Director: Ang Lee.
Brutally obvious "message" film-making just doesn't get more effective and entertaining than Ang Lee's THE ICE STORM. Continuing the trend of "Me Decade" venality-bashing begun by BOOGIE NIGHTS, it tells the tale of two troubled families in suburban New Canaan, Connecticut circa Thanksgiving 1973. Ben Hood (Kevin Kline) is having an affair with his next-door neighbor Janey Carver (Sigourney Weaver) though neither one is sure exactly why; Ben's wife Elena (Joan Allen) tries not to acknowledge that she suspects anything. Meanwhile, 14-year-old Wendy Hood (Christina Ricci) experiments sexually with both of Janey's sons, Mike (Elijah Wood) and Sandy (Adam Hann-Byrd), while Wendy's older brother Paul (Toby Maguire) tries to find a girl who isn't more interested in his prep school roommate Francis (David Krumholtz).
It takes no time at all to figure out that THE ICE STORM is meant as a critical study of an era when all sense of stability and authority were crumbling in America. With the Watergate scandal in full flower, parents dabbling in wife-swapping and even the local minister (Michael Cumpsty) given to flirting with his flock, the film's young characters are left to fumble for their moral way without a compass. When the parents actually do attempt to offer guidance, it proves worse than useless. Janey catches Wendy and Sandy together, then launches into a lecture which somehow drifts into primitive anthropology; Ben's years-too-late facts of life speech to Paul primarily covers "self-abuse" in the shower. James Schamus' script (adapted from Rick Moody's novel) makes it abundantly clear that plenty of important things were left unsaid while suburban parents of the 1970s were trying to be pals with their kids and "find themselves."
It is a credit both to the exceptional cast and to Schamus' finely detailed script that THE ICE STORM doesn't come off like exactly the kind of lecture those teenagers desperately needed. Moments of cringe-inducing awkwardness -- the tentative sexual games of youth, ill-advised romantic advances, foolish attempts to recapture the irresponsibility of girlhood -- spill off the screen as characters scramble aimlessly in search of some sort of fulfillment. Particularly vivid is the exploration of teen sexuality, energized by the frank performances of Ricci, Wood and Hann-Byrd. The treatment is neither exploitative nor ignorant, recognizing adolescents as far from the neutered creatures represented by Sandy's G.I. Joe action figure. Every performer turns in funny, provocative work, adding layers of confusion, yearning and desperation to a story which easily could have become pedantic.
THE ICE STORM only gets clumsy in the scenes involving Paul, whose infatuation with a wealthy New York girl is the stuff of over-earnest coming of age dramas. Toby Maguire has an affable charm, but his character never feels fully integrated into the story; he's a nice-guy throwback whose acts of conscience function primarily as counterpoint to the mistakes made by the rest of his family. His physical remove from the action does end up working wonderfully in the powerful conclusion, however, as tragedy forces characters to face up to their self-absorption and realize what matters to them most. It's an obvious lesson, perhaps, but one delivered with skill and grace. All family values sermons should be this haunting and insightful.
On the Renshaw scale of 0 to 10 ice teases: 8.
Visit Scott Renshaw's MoviePage http://www.inconnect.com/~renshaw/ *** Subscribe to receive new reviews directly by email! See the MoviePage for details, or reply to this message with subject line "Subscribe".
The review above was posted to the
rec.arts.movies.reviews newsgroup (de.rec.film.kritiken for German reviews).
The Internet Movie Database accepts no responsibility for the contents of the
review and has no editorial control. Unless stated otherwise, the copyright
belongs to the author.
Please direct comments/criticisms of the review to relevant newsgroups.
Broken URLs inthe reviews are the responsibility of the author.
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Related links: index of all rec.arts.movies.reviews reviews


Hey guys! I’m back from Nationals and I played pretty well. I got to the quarterfinals of Men’s singles! (yay Teddy) But in Men’s singles, Men’s Doubles, and U-21 years old, I lost to the same guy who was the top seed in the tournament….so just a bad draw. I think in the quarterfinals if I played anyone else I would’ve had a good chance, but I can’t complain about the draw it’s not under my control. But yeah, top 8 in Men’s in US isn’t bad. 🙂
Vegas was really hot and they also had a lot of other events in the hall. There was like a national dance competition which actually looked even more boring than pingpong if that is possible, CombatCon which is a martial arts convention, a MMA competiton where the women looked like they could kill me in three seconds or less, and the world series of beer pong. The beer pong competition was legit. First place is $50,000. For real pingpong first place is $4,000. We should totally do it when we are 21.
I’m on my second midterm for my computer science course so we’re gonna see how that goes but this time the material was quite harder. I think I will switch to computer science since I like it.
Otherwise, nothing much has changed…just chilling, waiting for the original bub to come back. I’m pretty psyched for college it’s only like 5 weeks away. Not too much to update on, so peace!


Official Statistics
The Programme for International Student Assessment (PISA) is an international survey of educational achievement organised by the Organisation for Economic Co-operation and Development (OECD).
Ref: OSR29/2010 Plain text , 820Bytes
If you use assistive technology (such as a screen reader) and need a version of this document in a more accessible format, please email<EMAIL_ADDRESS>. Please tell us what format you need. It will help us if you say what assistive technology you use.
PDF , 72.4KB , 17 pages
If you use assistive technology (such as a screen reader) and need a version of this document in a more accessible format, please email<EMAIL_ADDRESS>. Please tell us what format you need. It will help us if you say what assistive technology you use.
Reference Id: OSR29/2010
Publication Type: Statistical Release
Region: England
Release Date: 07 December 2010
Coverage status: Final
Publication Status: Published
PISA assesses the knowledge and skills of students aged fifteen and is carried out on a 3-year cycle, with each cycle assessing reading, mathematics and science and focusing mainly on one of these three areas. The ‘major domain’ of PISA 2009 is reading. The PISA publication was released at 10am on 7 December to coincide with the wider release of information across Europe and elsewhere. The Department normally releases official statistics at 9.30am.
Steve Leman
0114 274 2139


We are implementing an end-to-end pipeline that will be capable of doing real-time pedestrian path prediction. Given a scene with pedestrians walking through it, our system will be able to predict the path each pedestrian will take through the scene. Because the steps involved in this are quite computationally intensive, we will be using an FPGA to accelerate the pipeline, which should allow us to run it in real time.
This system has applications in many different areas. Successful path prediction will allow engineers to analyze foot traffic in public spaces such as train stations to help ease congestion. Pedestrian movement prediction can also be used for collision avoidance in autonomous vehicles. More generally, human behavior prediction can be used to do things like optimize the positioning of products in large stores. Outside of engineer, a system like this could also be used for applications like sports analysis, where coaches could predict the movements of players in different formations and use that data to come up with team tactics.
There are 4 major parts of our system: Object/Person Detector, Path Predictor, Programmable Logic (FPGA on Zedboard), User Interface. The Object Detector will use HOG features to detect pedestrians in a frame. The Path Predictor will use Linear Regression to predict the pedestrians path given their current position and history of positions in the video. The Programmable Logic will accelerate the computation of the Object Detector and Path Predictor. The User Interface will display our system's prediction in a visually pleasing way.
The diagram below outlines our high-level architecture.
The table below shows the work distribution for this project. The key task categories match up to those found in the Gantt chart below.
| Task Category | Atulya | Andres | Felix |
|---|---|---|---|
| Research | |||
| Preparation | |||
| Object Detector | |||
| Path Predictor | |||
| Hardware Acceleration | |||
| User Interface | |||
| Integration |
Below is our planned schedule for the Spring 2018 semester. The Gantt chart outlines each of the tasks that need to be completed along with their expected duration.


Cosmic Explorer Science Letters
In May 2023, the Cosmic Explorer Project requested Science Letters to support our community response to ngGW, the NSF Directorate for Mathematical & Physical Sciences Next-Generation Gravitational Wave Observatory Subcommittee. The ngGW Subcommittee had been asked to recommend GW detection network configurations that will deliver a detector with sensitivity an order of magnitude greater than the LIGO A+ design. The Cosmic Explorer community response included the following Letters:
- C. Fryer, GW Compact Remnant Mass Constraints as Probes of the Supernova Engine, CE-P2300002
- L. van Son et al., What we need from XG observatories to unveil the birth, life and death of massive stars – Part 1: births, CE-P2300014
- F. Broekgaarden et al., What we need from XG observatories to unveil the birth, life and death of massive stars – Part 2: life, CE-P2300015
- L. van Son et al., What we need from XG observatories to unveil the birth, life and death of massive stars – Part 3: stellar death, CE-P2300016
- I. Bartos et al., Orbital Eccentricity as the Fingerprint of Merger Origin, CE-P2300010
- T. Mishra et al., Probing black hole growth with Intermediate mass black holes, CE-P2300011
- P. Landry et al., Next-generation dense matter science with binary neutron star inspirals, CE-P2300013,
- E. R. Most and C. A. Raithel, Resolving Phase Transitions in the Neutron Star Equation924 of State, CE-P2300006
- A. Haber, M. G. Alford and E. R. Most, How Third Generation Gravitational Wave Detectors Can Unveil the True Degrees of Freedom of Dense Matter, CE-P2300004
- C. A. Raithel and V. Paschalidis, New Probes of the Finite-Temperature Dense-Matter Equation of State with Cosmic Explorer, CE-P2300012
- R. Sambruna, F. Civano and B. Humensky, Synergies of future ground-based GW detectors with space assets for multi messenger Astrophysics, CE-L2300011
- E. Murphy et al., Synergies between Cosmic Explorer and the ngVLA, CE-P2300009
- S. Gossan and E. D. Hall, Optimizing XG detector networks for Galactic astrophysics, CE-P2300017
- O. Gottlieb, Detecting Gravitational-waves from Collapsar Cocoons with the Cosmic Explorer, CE-P2300003
- M. Ball and R. Frey, Galactic Magnetars and Cosmic Explorer, CE-P2300010
- A. Grant et al., Gravitational-Wave Memory Effects in XG Observatories, CE-L2300012
- H. -J. Kuan et al., Gravitational phase transitions with Cosmic Explorer, CE-P2300007
- R. Essick and M. Isi, Distinguishing scalar gravitational-wave polarizations with next-generation detectors, CE-P2300008
- S.-J. Jin, Forecast for cosmological parameters in the era of the third-generation gravitational-wave detectors, CE-P2300005
These Letters, and their exploration of the science potential of Cosmic Explorer, were an esential contribution to the development of the Cosmic Explorer White Paper to be submitted to ngGW for the June 12 deadline.
Call for Science Letters
The NSF Directorate for Mathematical & Physical Sciences has asked the Next-Generation Gravitational Wave Observatory Subcommittee (ngGW) to recommend GW detection network configurations that will deliver a detector with sensitivity an order of magnitude greater than the LIGO A+ design. The Cosmic Explorer Project is requesting Science Letters to support our community response to ngGW.
Science Letters are informal public documents that will explore the scientific potential of next-generation (XG) gravitational-wave observatory networks. Each Science Letter should outline the capabilities and timelines needed for an XG network to address a specific science question. Science Letters are encouraged to suggest benchmarks that will ensure that the XG network is capable of the breakthrough science that they describe.
An XG network may include a combination of Cosmic Explorer, Einstein Telescope, Nemo, and upgraded detectors in current and planned ~4km-scale facilities (LIGO-US, LIGO-India, Virgo, KAGRA). Science Letters should focus on desired observational capabilities rather than specific sites or configurations.
Each Science Letter should contain a maximum of 2 pages of text and figures, as well as authors and relevant references. They should use clear and straightforward language that is understandable for scientists from a variety of fields. Contact information (names and email address) for corresponding Authors should be included in the Science Letter. Information for additional endorsing Authors may also be included.
Our ngGW White Papers (pdf) will draw from benchmarks in the Science Letters for network comparisons and science traceability. Cosmic Explorer White Paper teams may be recruited based on Science Letter authorship. Science Letters do not preclude independent White Paper authorship.
We encourage all members of the Cosmic Explorer Consortium to collaborate on Science Letters and to engage early career researchers and graduate students in the process. Science Letters that include authors with diverse backgrounds, perspectives, and experiences are essential. Authors do not need to be Consortium members. You may list letters in progress and points of contact in this spreadsheet to encourage collaboration and coordination.
Science Letters should be uploaded to the Cosmic Explorer DCC and added to the Science Letters Event or submitted using this CE Science Letter Form. Letters are requested by May 8 to best enable their use in White Papers.
Thank you in advance for your contributions! We look forward to reading your Science Letters, and to working together to advance our understanding of the Universe through gravitational-wave observations.
FAQ
Is there a recommended format?
We have a suggested Overleaf Template that we encourage you to use.
What are benchmarks?
A benchmark should represent a desired observational capability, such as detection rate or sensitivity, that can be used to differentiate between potential XG networks. Science Letters should explain how reaching certain benchmarks would ensure that gravitational-wave astronomy contributes to new knowledge pathways.
Example benchmarks could include:
- Characteristic strain sensitivity between 10 and 100 Hz.
- Number of sources with 10 deg2 localization available 5 minutes before merger.
- Number of BBH mergers detected per year with SNR > 600.
- Horizon distance for BNS observations relative to peak star formation redshift.
- Number of BBH and BNS detected at redshift larger than 2.
- Integrated 1-year sensitivity to stochastic backgrounds with a fractional energy density ΩGW(f) in gravitational waves .
- Sensitive range for a burst that releases EGW of 10-9 M⊙c2 at 1 kHz.
- Ellipticity of known pulsars with measurable quadrupole emission.
- Sensitive range for a long-duration source of some characteristic timescale and hRSS.
The potential scale of XG network capabilities can be seen in studies including [2109.09882] A Horizon Study for Cosmic Explorer: Science, Observatories, and Community and [2303.15923] Science with the Einstein Telescope: a comparison of different designs.
What detector network or locations should I use?
Because the exact configuration of the ngGW network is in active development, we ask that Science Letters focus on desired observational requirements instead of specific detector locations and configurations. White Paper teams may later reach out to Science Letter authors to collaborate on assessing the science capabilities of candidate networks.
What topics might science letters address?
- Key science questions addressed by gravitational-wave observations of mergers, unmodeled transients, long-duration or continuous signals, and stochastic backgrounds.
- Multi-messenger astronomy potential with gravitational waves, including joint observations with other telescopes and detectors.
- Potential contributions of XG observatories to open questions in areas including cosmology, high energy physics, particle physics, and nuclear physics.
- Interdisciplinary impacts of XG development, such as applications in materials science, data science, or quantum optics.
- Neglected or overlooked areas of XG science with high potential impact.
Where can I ask additional questions?
Please reach out to Jocelyn Read (jread AT fullerton.edu) and Salvatore Vitale (svitale AT mit.edu) with any questions about the Science Letters.


Registering Hextrapolate
Once you have purchased a Hextrapolate license you will receive a license code via email. To complete the registration you will copy your license code from the email into Hextrapolate.
To register your copy of Hextrapolate:
- From the Hextrapolate menu select Register…
- When the registration preference pane appears, click the “Enter license code” button
- When the confirmation sheet drops down, enter your email address exactly as it appears in your license notice (if you enter a different address your license will not work) into the text field labelled “Email address”
- In the field labelled “License code”, enter your license code exactly as it appears in your license notice; license codes are quite long so the best way to do this is to use copy and paste (you can copy the entire code at once as a single slab of text)
- Click the Verify button to activate your license


Careers
Working for LYT Systems provides an unique experience. If you want to strive to work in an organization
where you can show talentand enhance your skills? LYT Systems is where you belong.
Benefits
- Medical Insurance – 100% company paid
- Dental Insurance – 100% company paid
- Vision Care – 100% company paid
- Short Term Disability
- Long Term Disability
- Life Insurance
- Tuition reimbursement
- Yearly Bonuses
- 401k- 6% dollar to dollar match and vested immediately
- Paid training
- Yearly allowance for technical purchases
- Health and wellness Allowance
Openings
- Software developers with specializations in:
- AWS Cloud Computing
- Spring
- Web developer


Open San Diego National Day of Civic Hacking¶
Open San Diego’s activity for NDoCH will be anchored around a day of presentations and hands-on participation for all levels of experience. This is the fourth year of National Day. In years prior, government representatives have made appearances across the country. These have included everyone from top-ranking White House Officials, to Governors, Mayors and Fire Department Chiefs. Our featured speaker this year will be City Councilmember Todd Gloria. We are also honored to have presentations from Brian Genovese, Senior Engineer, Transportation and Storm Water, City of San Diego; and the City’s Chief Data Officer Maksim Percheskiy. Both Mr. Percheskiy and the City’s Performance and Analytics Department, where he works, are the official Municipal Partners of the Open San Diego, Code for America Brigade.
Open San Diego’s National Day will be family-friendly, with engaging activity for programmers, parents and children, urbanists, designers, municipal staff, makers,, students and anyone else interested in presentations and hands-on activities focused on making the lives of San Diegans better.
A “Hack” is a fast solution to a problem. It’s fast to conceive and it’s fast to execute. It may not be the perfect solution, but it’s a step we take that gets us to perfect, faster. Here are the kinds of “hacks” will be pursuing at the different event sites. All activity, including satellite events will take place between 10am and 4pm, although activity at some sites will end earlier than 4pm.
Spread over three four locations and three neighborhoods our hacks for the day will include community asset mapping, coding lessons for youth, neighborhood prototyping, food trucks, community collaboration enabled by DIY radio Broadcasts and community organizing efforts
Open San Diego’s community partners for the event are: - Fab Lab San Diego, - the Placemaking Collective, - the Elementary Institute of Science, - the Jacobs Center, - The Urban Collaborative Project, and the - City of San Diego.
The Sites¶
Downtown/East Village | Fab Lab San Diego: Prototyping Communities Site | 847 14th St, San Diego, California 92101| 10am – 4pm Hacking the spaces where we live and play for Change:
- Code lessons for kids,
- Neighborhood Prototyping using digital mapping tools to add the elements you think would improve your neighborhood.
- Attendees may also participate in developing new Civic Tech tools from Open San Diego::
- a crowdsourcing app that helps parents identify the best recreation areas for their kids,
- a personal notification tool for people interested in local development projects,
- a civic engagement app aimed at increasing the benefits of street sweeping.
City Heights | Placemaking Collective @ AjA Project : Bicycle Safety and Advocacy Site | 4089 Fairmount Ave, San Diego, California 10am – 1pm Hacking Transportation Infrastructure for Change Participants (technical and non-technical) will collaborate to define the most pressing needs of the bike community and then work together to produce an app that meets those needs, based on this version produced by the Philly Brigade: http://bit.ly/cycle_app_news.
Encanto | San Diego Futures Foundation + Elementary Institute of Science: Paving Community Careers Pathways Site | 608 51st St, San Diego California. 10am – 2pm Hacking Education for Change
The Diamond | Jacobs Center + The Urban Collaborative Project: Inter-Community Communications Corner of Market and Imperial (Jun 5) 5pm – 7pm Hacking Community Collaboration for Change


11+ Wood Logs For Smoking Meat Near Me Pics. Choosing the best wood for smoking and grilling for more barbecue and grilling recipes visit: Good with red meats and game.
You can balance cherry wood by mixing it with hickory, oak, or. Cherry hard wood logs perfect for smoking or as a firewood seasoned 5 years. When smoking meat on the barbecue, having great quality meat helps!
Cherry hard wood logs perfect for smoking or as a firewood seasoned 5 years.
Wood chunks are especially useful for smoking meat because of their size. When smoking meat on the barbecue, having great quality meat helps! These are best reserved for barbecuing in a pit or with an offset smoker, but we're talking grilling, and i the mild woods pair best with more delicate meats like chicken and fish, where a little smoke goes a long way. These hickory wood logs are ideal for smoking red meat, duck, lamb, and poultry.


'Network'
A retrospective movie review by Walter Frith
Member of the 'Internet Movie Critics Association' http://www.geocities.com/Hollywood/Studio/5713/index.html
Uggh, tabloid t.v. Catering to the lowest common denominator. That's nothing new. Before the trashy antics of these sleaze profiteers there were other, more innocuous attempts to get people hooked on boob tube entertainment of a low class nature. 'The Gong Show' perhaps? The 'Unknown Comic', 'Gene, Gene, the dancing machine' and that curly haired host were all bad enough but 20 years ago who would have thought that during a television talk show, fights would break out. Now it seems that during fights on these shows, audiences keep waiting for a talk show to break out. When Geraldo had his nose broken some years ago, many thought that sort of thing was the exception rather than the rule and while few people get injured on these shows, at least what the audience sees first hand, I truly believe that these scenarios are REAL! Perhaps not all the time, but surely the famous incident involving the murder of a young man by another man as an alleged result of appearing on one of these shows, makes you wonder how much is staged and how much is indeed real. In case you don't know what I'm talking about, there was an incident a couple of years ago where a certain trash talk show had people on stage waiting to meet their secret admirers.  You can guess the rest.
In 1976, when the film 'Network' came out, it was about a fourth place network, UBS, and ABC, NBC, and CBS all finishing ahead of it in the ratings each week. Desperate to get ratings and offset huge annual financial losses, they luck into something. A washed up television anchor man named Howard Beale (Peter Finch, in his Oscar winning role as Best Actor), has his employment terminated because of low ratings and announces during a live broadcast that he will commit suicide on live television in the near future before he leaves for good. Causing panic among the executives watching, they remove him by force and after some thought, Beale convinces another executive and his best friend, Max Schumacher (William Holden), to put him back on to rectify the embarrassing statement. Given this opportunity, he causes more embarrassment for the network by using the word "bull****" and the ratings jump 5 points during that broadcast. Taking advantage of this situation, a ruthless female executive named Diana Christensen (Faye Dunaway in her Oscar winning role as Best Actress), convinces her boss in charge of programming, Frank Hackett (Robert Duvall) to put Howard Beale back on the air and keep him on despite the irresponsible nature of his content and the shocking nature of his messages. He agrees and thus 'The Howard Beale Show' is born. He is described and an 'angry prophet, denouncing the hypocrisies of our time'. His show influences the network to include other tabloid segments and this shocking new brand of television causes a fury among angry broadcast regulators and government officials who want the show stopped.
Screenwriter Paddy Chayefsky, who won his third Oscar for the scathing script of 'Network' was a true genius way ahead of his time. He predicted back then that television standards would get lower and lower and they most definitely have. In addition to tabloid talk shows, people have to contend with sitcoms that all look the same, recycled from ideas of the past without a clue in proper execution or hint of original thought. '3rd Rock from the Sun'/'Mork and Mindy', 'Frasier'/'Cheers'. Even highly charged dramas such as 'ER' and 'NYPD Blue' bring up memories of 'St. Elsewhere' and 'Hill Street Blues'. Chayefsky's observations of television programming are not cynical, just the thoughts of a realist. For all of you doubting Thomas' out there, ask yourself why many shows debut in the fall while only two or three survive after the first year.

Nominated for 10 Oscars in 1976, including Best Picture and Best Director (Sidney Lumet), 'Network', as I mentioned, won Best Actor and Actress Oscars for Peter Finch and Faye Dunaway. Finch died before the awards were given out and received his award posthumously. In addition to the acting awards won by Finch and Dunaway, Beatrice Straight won the Best Supporting Actress Oscar as Max Schumacher's tortured wife living with the reality that her husband is in love with and is having an affair with another woman. Straight's performance is an example of why the Supporting acting categories were created. She only appears in a couple of scenes but they are brimming with talent and a convincing portrayal of her character. The most unique performance in 'Network' comes from Ned Beatty who plays the top executive in the television company who delivers his philosophy of the corporate world like a television evangelist. He received a Best Supporting Actor nomination and finally, William Holden was nominated along side Finch for Best Actor. Not many films get the distinction of having five cast members nominated for Oscars, and as of 1997, 'Network' and 1951's 'A Streetcar Named Desire' remain the only two films to receive three Academy Awards for acting.
Visit FILM FOLLOW-UP by Walter Frith http://home.netinc.ca/~wfrith/movies.htm
The review above was posted to the
rec.arts.movies.reviews newsgroup (de.rec.film.kritiken for German reviews).
The Internet Movie Database accepts no responsibility for the contents of the
review and has no editorial control. Unless stated otherwise, the copyright
belongs to the author.
Please direct comments/criticisms of the review to relevant newsgroups.
Broken URLs inthe reviews are the responsibility of the author.
The formatting of the review is likely to differ from the original due
to ASCII to HTML conversion.
Related links: index of all rec.arts.movies.reviews reviews


Blacksmith Duning:
Sorry about that. The sequence was gold - silver - blood. Don't be discouraged. You can't win them all!


Retrieve a MARC21 or PICA+ record from K10plus Union Catalog and analyze an Avram Schema based on its fields. See avram-js for implementation.


--- layout: post title: banana ginger chocolate chip softies date: 2012-05-14 23:35:33.000000000 -04:00 type: post published: true status: publish categories: - cookies - vegan tags: - banana - chocolate chip - cookies - fat free - ginger - vegan meta: _edit_last: '1' author: login: sophie email<EMAIL_ADDRESS>display_name: Pika first_name: '' last_name: '' ---
Ah, home sweet home! After a grueling exams week, I'm finally back in Jersey. Well, for a week at least--I move in to start my summer fellowship program Sunday (more on that later).
Of course I put no time to waste in indulging in all the best things about break: banana chocolate-chip pancakes for breakfast, slurping down my favorite banana-cocoa smoothies twice a day, taking the scissors to the closet, lovingly harassing the cat, taking 3-hour naps, and watching many re-runs of that 70's show. And, naturally, baking cookies!
I adore candied ginger and these cookies were inspired by my addiction to the spicy sweet taste. I used mini chocolate chips for more uniform chocolate per bite (it's all about the math, folks). Because they don't contain any added fat or egg, these cookies end up being very, very moist, which is a great thing taste-wise, but not so great if you want to transport or store them for too long. So eat 'em while they're warm and spicy, with a friend or two to share with!
Ginger Chocolate-Chip Banana Softies
Makes about 16 cookies
Adapted from VegWeb
1 ¼ c whole wheat flour
½ t baking soda
½ t salt
1 very ripe banana
½ c unsweetened applesauce (1 snack-pack)
½ c sugar
1 t vanilla
½ c crystallized ginger, chopped
⅓ c mini chocolate chips


The No-Go Theorems of Quantum Information Theory (Part 2)
Introduction
A couple of weeks ago, I started a high-level overview of some of the no-go theorems in quantum information theory. In that first post, we covered the no-cloning theorem, the no-teleportation theorem, and the no-hiding theorem. The no-cloning theorem states that we cannot copy an arbitrary qubit using a unitary operator. The no-teleportation theorem states that we cannot determine an arbitrary quantum state with just one measurement. Finally, the no-hiding theorem states that quantum information is never truly lost; instead, the information only moves between our system and the environment.
This week, we will focus on two more no-go theorems in quantum information theory.
###The No-Deletion Theorem
The no-deletion theorem in quantum information theory states given two copies of some arbitrary quantum state, it is impossible to delete one of the copies against the other. In other words, there is no unitary operator \(U\) such that:
\[\begin{equation} U \left ( | \psi \rangle | \psi \rangle | \phi \rangle \right )= | \psi \rangle | 0 \rangle | \phi' \rangle \end{equation}\]In the expression above, \(\phi\) and \(\phi'\) are two general strings of qubits before and after the operation. They are simply written above for completeness.
The proof of this theorem is straightforward and similar to that of the no-cloning theorem. Suppose there did exist a unitary operator \(U\) that could be used to perform a deletion as stated above. Then:
\[\begin{equation} U \left ( | 0 \rangle | 0 \rangle | \phi \rangle \right )= | 0 \rangle | 0 \rangle | \phi' \rangle \end{equation}\] \[\begin{equation} U \left ( | 1 \rangle | 1 \rangle | \phi \rangle \right )= | 1 \rangle | 0 \rangle | \phi' \rangle \end{equation}\]We can define an arbitrary state \(\psi\) as:
\[\begin{equation} | \psi \rangle = a |0\rangle + b|1\rangle \end{equation}\]On the one hand:
\[\begin{align} U \left ( | \psi \rangle | \psi \rangle | \phi \rangle \right ) &= | \psi \rangle | 0 \rangle | \phi' \rangle\\[0.1cm] &= a | 0 \rangle | 0 \rangle | \phi' \rangle + b | 1 \rangle | 0 \rangle | \phi' \rangle \end{align}\]But on the other hand:
\[\begin{align} U \left ( | \psi \rangle | \psi \rangle | \phi \rangle \right ) &= U \left [ \left ( a | 0 \rangle + b | 1 \rangle \right ) \left ( a | 0 \rangle + b | 1 \rangle \right ) | \phi \rangle \right ]\\[0.1cm] &= U \left [ a^2 | 0 \rangle | 0 \rangle + b^2 | 1 \rangle | 1 \rangle + ab | 0 \rangle | 1 \rangle + ba | 1 \rangle | 0 \rangle \right ] | \phi \rangle\\[0.1cm] &= a^2 U| 0 \rangle | 0 \rangle | \phi \rangle + b^2 U| 1 \rangle | 1 \rangle | \phi \rangle + ab U| 0 \rangle | 1 \rangle | \phi \rangle + ba U| 1 \rangle | 0 \rangle | \phi \rangle\\[0.1cm] &= a^2 | 0 \rangle | 0 \rangle | \phi' \rangle + b^2 | 1 \rangle | 0 \rangle | \phi' \rangle + ab U \left ( | 0 \rangle | 1 \rangle + | 1 \rangle | 0 \rangle \right ) | \phi \rangle\\[0.1cm] \end{align}\]The last part of the expression is an entangled state. We can define it as \(\Phi\):
\[\begin{align} U \left ( | \psi \rangle | \psi \rangle | \phi \rangle \right ) &= a^2 | 0 \rangle | 0 \rangle | \phi' \rangle + b^2 | 1 \rangle | 0 \rangle | \phi' \rangle + ab U | \Phi \rangle | \phi \rangle\\[0.1cm] \end{align}\]Thus, we see a contradiction. In the first calculation, the final state is defined in terms of a, b, 0, 1, and \(\phi'\). But in the other calculation, we see an additional entangled state in the final expression. The two calculations are not equal in general, and \(U\) cannot exist (proof by contradiction).
This theorem is important because it shows how quantum states are not as fragile as they seem. In general, we think about how quantum states can lose coherence due to even minor environmental interference. But here, we see that quantum states might be able to last in certain circumstances.
###The No-Communication Theorem
This is an unfortunately named theorem. It does not state that communication is impossible using quantum systems. Rather, it says that information cannot travel faster than the speed of light. This statement comes directly from the special theory of relativity.
How does this relate to quantum information theory specifically? About one decade ago, scientists discovered that when they created an entangled pair of qubits called a Bell state, separated them, and measured them against each other, the information about the state of the system seemed to travel between them instantaneously. The quantum information community did not quite know how to deal with this situation; it seemed like the information about the two qubits were traveling between them faster than the speed of light. Does this violate the no-communication theorem?
It turns out that it does not. Suppose Alice prepares an entangled pair of qubits in a Bell state. She takes one of the qubits and gives Bob the other, without telling him any details about the initial preparation. Finally, Alice measures her qubit and collapses the state. What can Bob say about the original state of the qubits? Effectively nothing. He has no idea if it was an entanlged state or simply a product state. Thus, even though the qubits “communicate” the collapse of the state seemingly faster than the speed of light, Bob cannot glean any useful information about the state from his measurement. Another way to state this theorem is one cannot transmit information using entanglement alone.
Next Week
Next week, we will first take a bit of time to discuss the partial trace of a quantum system. Then, we will use that information to finish the discussion of the no-go theorems in quantum information theory. Until next week!


public class TdApi
extends java.lang.Object
It has no inner classes, functions or public members.
| Modifier and Type | Class and Description |
|---|---|
static class |
TdApi.AddChatParticipant
Add new participant to chat.
|
static class |
TdApi.Audio
Describes audio file.
|
static class |
TdApi.AuthGetState
Returns current authorization state, offline request.
|
static class |
TdApi.AuthReset
Logs out user.
|
static class |
TdApi.AuthSetCode
Sets authorization code.
|
static class |
TdApi.AuthSetName
Sets user first_name and last_name.
|
static class |
TdApi.AuthSetPhoneNumber
Sets user's phone number and sends authorization code to user.
|
static class |
TdApi.AuthState
This class is an abstract base class.
|
static class |
TdApi.AuthStateLoggingOut
User is currently logging out.
|
static class |
TdApi.AuthStateOk
User is successfully authorized.
|
static class |
TdApi.AuthStateWaitSetCode
TDLib needs user authorization code to finish authorization.
|
static class |
TdApi.AuthStateWaitSetName
User is authorized first time.
|
static class |
TdApi.AuthStateWaitSetPhoneNumber
TDLib needs user's phone number to authorize.
|
static class |
TdApi.BlockUser
Add user to black list.
|
static class |
TdApi.CancelDownloadFile
Stops file downloading.
|
static class |
TdApi.ChangeChatTitle
Change chat title.
|
static class |
TdApi.Chat
Chat (group chat or secret chat or private chat).
|
static class |
TdApi.ChatInfo
This class is an abstract base class.
|
static class |
TdApi.ChatParticipant
User with information about its chat joining.
|
static class |
TdApi.Chats
Contains list of chats.
|
static class |
TdApi.Contacts
User contacts.
|
static class |
TdApi.CreateGroupChat
Create group chat and send corresponding messageGroupChatCreate, returns created chat.
|
static class |
TdApi.CreatePrivateChat
Create private chat with one interlocutor.
|
static class |
TdApi.DeleteChatHistory
Deletes all messages in a chat.
|
static class |
TdApi.DeleteChatParticipant
Kick participant from chat or left a chat.
|
static class |
TdApi.DeleteMessages
Delete messages.
|
static class |
TdApi.Document
Describes document.
|
static class |
TdApi.DownloadFile
Asynchronously download file from cloud.
|
static class |
TdApi.Error
Object of this type may be returned on every function call in case of error.
|
static class |
TdApi.File
This class is an abstract base class.
|
static class |
TdApi.FileEmpty
Nonavailaible cloud file.
|
static class |
TdApi.FileLocal
Local file.
|
static class |
TdApi.ForwardMessages
Forward previously sent messages.
|
static class |
TdApi.GeoPoint
Describes location on Earth.
|
static class |
TdApi.GetChat
Returns information about chat by its identifier, offline request.
|
static class |
TdApi.GetChatHistory
Returns messages in a chat.
|
static class |
TdApi.GetChats
Returns information about chats.
|
static class |
TdApi.GetContacts
Returns user contacts list.
|
static class |
TdApi.GetGroupChat
Returns information about group chat by its identifier, offline request.
|
static class |
TdApi.GetGroupChatFull
Returns full information about group chat by its identifier.
|
static class |
TdApi.GetMe
Returns current logged in user, offline request.
|
static class |
TdApi.GetNotificationSettings
Returns notification settings for given scope.
|
static class |
TdApi.GetOption
Returns value of an option by its name.
|
static class |
TdApi.GetStickers
Returns stickers corresponding to given emoji.
|
static class |
TdApi.GetUser
Returns information about user by its identifier, offline request.
|
static class |
TdApi.GetUserFull
Returns full information about user by its identifier.
|
static class |
TdApi.GroupChat
Represents a chat with zero or more other users.
|
static class |
TdApi.GroupChatFull
Gives full information about group chat.
|
static class |
TdApi.GroupChatInfo
Chat with zero or more other users.
|
static class |
TdApi.InputMessageAudio
Audio message.
|
static class |
TdApi.InputMessageContact
User contact message.
|
static class |
TdApi.InputMessageContent
This class is an abstract base class.
|
static class |
TdApi.InputMessageDocument
Document message.
|
static class |
TdApi.InputMessageForwarded
Forwarded message.
|
static class |
TdApi.InputMessageGeoPoint
GeoPoint message.
|
static class |
TdApi.InputMessagePhoto
Photo message.
|
static class |
TdApi.InputMessageSticker
Sticker message.
|
static class |
TdApi.InputMessageText
Text message.
|
static class |
TdApi.InputMessageVideo
Video message.
|
static class |
TdApi.LinkState
This class is an abstract base class.
|
static class |
TdApi.LinkStateContact
Other user is in contacts list, particularly its phone number is known.
|
static class |
TdApi.LinkStateKnowsPhoneNumber
Other user's phone number is known but user not in contacts list.
|
static class |
TdApi.LinkStateNone
Other user's phone number doesn't known.
|
static class |
TdApi.Message
Describes message.
|
static class |
TdApi.MessageAudio
Audio message.
|
static class |
TdApi.MessageChatAddParticipant
Chat participant added.
|
static class |
TdApi.MessageChatChangePhoto
Chat photo changed.
|
static class |
TdApi.MessageChatChangeTitle
Chat title changed.
|
static class |
TdApi.MessageChatDeleteParticipant
Chat participant deleted.
|
static class |
TdApi.MessageChatDeletePhoto
Chat photo deleted.
|
static class |
TdApi.MessageContact
User contact message.
|
static class |
TdApi.MessageContent
This class is an abstract base class.
|
static class |
TdApi.MessageDeleted
Message was deleted or was never existed.
|
static class |
TdApi.MessageDocument
Document message.
|
static class |
TdApi.MessageGeoPoint
Message with GeoPoint.
|
static class |
TdApi.MessageGroupChatCreate
New group chat created.
|
static class |
TdApi.MessagePhoto
Photo message.
|
static class |
TdApi.Messages
Contains list of messages.
|
static class |
TdApi.MessageSticker
Sticker message.
|
static class |
TdApi.MessageText
Text message.
|
static class |
TdApi.MessageUnsupported
Unsupported message content.
|
static class |
TdApi.MessageVideo
Video message.
|
static class |
TdApi.NotificationSettings
Contains information about notification settings for chat or chats.
|
static class |
TdApi.NotificationSettingsForAllChats
Notification settings applied to all chats.
|
static class |
TdApi.NotificationSettingsForChat
Notification settings applied to particular chat.
|
static class |
TdApi.NotificationSettingsForGroupChats
Notification settings applied to all group chats.
|
static class |
TdApi.NotificationSettingsForPrivateChats
Notification settings applied to all private chats.
|
static class |
TdApi.NotificationSettingsScope
This class is an abstract base class.
|
static class |
TdApi.Ok
Object of this type returns on successful function call for some functions.
|
static class |
TdApi.OptionBoolean
Boolean option.
|
static class |
TdApi.OptionEmpty
Unknown option or option having default value.
|
static class |
TdApi.OptionInteger
Integer option.
|
static class |
TdApi.OptionString
String option.
|
static class |
TdApi.OptionValue
This class is an abstract base class.
|
static class |
TdApi.Photo
Describes photo.
|
static class |
TdApi.PhotoSize
Photo description.
|
static class |
TdApi.PrivateChatInfo
Ordinary chat with one user.
|
static class |
TdApi.SendMessage
Send text message.
|
static class |
TdApi.SendMessageAction
This class is an abstract base class.
|
static class |
TdApi.SendMessageCancelAction
User cancels typing.
|
static class |
TdApi.SendMessageChooseContactAction
User chooses contact to send.
|
static class |
TdApi.SendMessageGeoLocationAction
User sends geolocation.
|
static class |
TdApi.SendMessageRecordAudioAction
User records an audio.
|
static class |
TdApi.SendMessageRecordVideoAction
User records a video.
|
static class |
TdApi.SendMessageTypingAction
User typing message.
|
static class |
TdApi.SendMessageUploadAudioAction
User uploads an audio.
|
static class |
TdApi.SendMessageUploadDocumentAction
User uploads a document.
|
static class |
TdApi.SendMessageUploadPhotoAction
User uploads a photo.
|
static class |
TdApi.SendMessageUploadVideoAction
User uploads a video.
|
static class |
TdApi.SetNotificationSettings
Changes notification settings for given scope.
|
static class |
TdApi.SetOption
Sets value of an option.
|
static class |
TdApi.Sticker
Describes sticker.
|
static class |
TdApi.Stickers
Represents set of stickers.
|
static class |
TdApi.TLFunction
This class is a base class for all TDLib interface function-classes.
|
static class |
TdApi.TLObject
This class is a base class for all TDLib interface type-classes.
|
static class |
TdApi.UnblockUser
Remove user from black list.
|
static class |
TdApi.UnknownGroupChatInfo
Chat with zero or more other users, but there is no other information about chat.
|
static class |
TdApi.UnknownPrivateChatInfo
Ordinary chat with one user, but there is no information about interlocutor.
|
static class |
TdApi.Update
This class is an abstract base class.
|
static class |
TdApi.UpdateChatParticipantsCount
Chat participants was changed.
|
static class |
TdApi.UpdateChatReadInbox
User reads incoming messages from some other device.
|
static class |
TdApi.UpdateChatReadOutbox
Some outcoming messages was read.
|
static class |
TdApi.UpdateChatTitle
Title of chat was changed.
|
static class |
TdApi.UpdateDeleteMessages
Some messages was deleted.
|
static class |
TdApi.UpdateFile
File is downloaded.
|
static class |
TdApi.UpdateFileProgress
File is partly downloaded.
|
static class |
TdApi.UpdateMessageContent
Sent message gets new content.
|
static class |
TdApi.UpdateMessageDate
Sent message gets new date.
|
static class |
TdApi.UpdateMessageId
Sent message gets persistent unique identifier.
|
static class |
TdApi.UpdateNewAuthorization
User has logged in from another device.
|
static class |
TdApi.UpdateNewMessage
New message received.
|
static class |
TdApi.UpdateNotificationSettings
Notification settings for some chats was updated.
|
static class |
TdApi.UpdateOption
Some option changed its value.
|
static class |
TdApi.UpdateStickers
Some stickers was updated.
|
static class |
TdApi.UpdateUserAction
Some chat activity.
|
static class |
TdApi.UpdateUserBlocked
User blocked/unblocked.
|
static class |
TdApi.UpdateUserLinks
Relationship with other user has changed.
|
static class |
TdApi.UpdateUserName
User changes its full name/username.
|
static class |
TdApi.UpdateUserPhoneNumber
User changes its phone number.
|
static class |
TdApi.UpdateUserPhoto
User changes its profile photo.
|
static class |
TdApi.UpdateUserStatus
User went online/offline.
|
static class |
TdApi.User
Represents user.
|
static class |
TdApi.UserFull
Gives full information about user (except full list of profile photos).
|
static class |
TdApi.UserStatus
This class is an abstract base class.
|
static class |
TdApi.UserStatusEmpty
User status was newer changed.
|
static class |
TdApi.UserStatusLastMonth
User is offline, but was online last month.
|
static class |
TdApi.UserStatusLastWeek
User is offline, but was online last week.
|
static class |
TdApi.UserStatusOffline
User is offline.
|
static class |
TdApi.UserStatusOnline
User is online.
|
static class |
TdApi.UserStatusRecently
User was online recently.
|
static class |
TdApi.Video
Describes video file.
|
| Constructor and Description |
|---|
TdApi() |


index page, (header) Includes,Title (Sidney's Photography), Site Navigation to Home,services,Contact Page, and About page, two images of the photographer (body) Includes, a paragraph about the photographer (footer) Includes, photographer name and phone number
Service Page, (header) Includes, Title (services), Site Navigation to Home,services,Contact Page, and About page, (body) Includes, Pricing for Couples, Seniors, Family, and Portrait, pictures for each, one review (footer) Includes, photographer name and phone number
Contact Me Page, (header) Includes, Title (services), Site Navigation to Home, services, Contact Page, and About page, one image (footer) photographer's name, email, and phone number
I did not include an image map becuase it does not go with my website. I did not add transparency (M4LO6 Demonstrate the use of opacity/transparency for images) my page is about photography and all images need to be at full opacity and transparency to be appreciated.
Index page, I took the images out of the header so I can use float and clear on them.
Services, I added an image for the Mini Sessions and made it a figure box (this will go away in v3).
Contact me, I added a gradient to the background. I also made a seperate stylesheet for this page.
On all pages, I added rounded corners to the bottom left and right corners and also added a text shadow to the address.
I did not include 'M5LO4 Use CSS for pull-down menus' becuase I found it unnecessary for my website.
Index Page, I moved the image back into the hearder where it was in v1 and added the second image back in.
Services, I got rid of the figure box becuase it did not flow with the simplicity of site. I added in more pictures for the mini sessions section of the page.
Contact Me, I addded a table to show the availability for the photographer's week.
Overall, on all pages I created the format for mobile and PCs and also added M5LO5, M5LO6, M5LO7 (those include- flex-direction, flex-wrap, flex-flow, width, height, flex, -webkit-order, -webkit-flex, -webkit-flex-flow, order, display)
I did not include the module 8 objectives because neither the iframe or annimation made sence to include into my project.
Contact Me, I added a Check List to give the option of recieving emails, Selection List to book a session, and a submit button to send the information to the photographer.
Services, I rearranged the photos and added more reviews.


\
We assume here that we are only interested in the ground state of the system and expand the exact wave function in term of a series of Slater determinants
$$
\vert \Psi_0\rangle = \vert \Phi_0\rangle + \sum_{m=1}^{\infty}C_m\vert \Phi_m\rangle,
$$
where we have assumed that the true ground state is dominated by the
solution of the unperturbed problem, that is
$$
\hat{H}_0\vert \Phi_0\rangle= W_0\vert \Phi_0\rangle.
$$
The state \( \vert \Psi_0\rangle \) is not normalized, rather we have used an intermediate
normalization \( \langle \Phi_0 \vert \Psi_0\rangle=1 \) since we have \( \langle \Phi_0\vert \Phi_0\rangle=1 \).
The Schroedinger equation is
$$
\hat{H}\vert \Psi_0\rangle = E\vert \Psi_0\rangle,
$$
and multiplying the latter from the left with \( \langle \Phi_0\vert \) gives
$$
\langle \Phi_0\vert \hat{H}\vert \Psi_0\rangle = E\langle \Phi_0\vert \Psi_0\rangle=E,
$$
and subtracting from this equation
$$
\langle \Psi_0\vert \hat{H}_0\vert \Phi_0\rangle= W_0\langle \Psi_0\vert \Phi_0\rangle=W_0,
$$
and using the fact that the both operators \( \hat{H} \) and \( \hat{H}_0 \) are hermitian
results in
$$
\Delta E=E-W_0=\langle \Phi_0\vert \hat{H}_I\vert \Psi_0\rangle,
$$
which is an exact result. We call this quantity the correlation energy.
This equation forms the starting point for all perturbative derivations. However, as it stands it represents nothing but a mere formal rewriting of Schroedinger's equation and is not of much practical use. The exact wave function \( \vert \Psi_0\rangle \) is unknown. In order to obtain a perturbative expansion, we need to expand the exact wave function in terms of the interaction \( \hat{H}_I \).
Here we have assumed that our model space defined by the operator \( \hat{P} \) is one-dimensional, meaning that
$$
\hat{P}= \vert \Phi_0\rangle \langle \Phi_0\vert ,
$$
and
$$
\hat{Q}=\sum_{m=1}^{\infty}\vert \Phi_m\rangle \langle \Phi_m\vert .
$$
We can thus rewrite the exact wave function as
$$
\vert \Psi_0\rangle= (\hat{P}+\hat{Q})\vert \Psi_0\rangle=\vert \Phi_0\rangle+\hat{Q}\vert \Psi_0\rangle.
$$
Going back to the Schr\"odinger equation, we can rewrite it as, adding and a subtracting a term \( \omega \vert \Psi_0\rangle \) as
$$
\left(\omega-\hat{H}_0\right)\vert \Psi_0\rangle=\left(\omega-E+\hat{H}_I\right)\vert \Psi_0\rangle,
$$
where \( \omega \) is an energy variable to be specified later.
We assume also that the resolvent of \( \left(\omega-\hat{H}_0\right) \) exits, that is it has an inverse which defined the unperturbed Green's function as
$$
\left(\omega-\hat{H}_0\right)^{-1}=\frac{1}{\left(\omega-\hat{H}_0\right)}.
$$
We can rewrite Schroedinger's equation as
$$
\vert \Psi_0\rangle=\frac{1}{\omega-\hat{H}_0}\left(\omega-E+\hat{H}_I\right)\vert \Psi_0\rangle,
$$
and multiplying from the left with \( \hat{Q} \) results in
$$
\hat{Q}\vert \Psi_0\rangle=\frac{\hat{Q}}{\omega-\hat{H}_0}\left(\omega-E+\hat{H}_I\right)\vert \Psi_0\rangle,
$$
which is possible since we have defined the operator \( \hat{Q} \) in terms of the eigenfunctions of \( \hat{H} \).
These operators commute meaning that
$$
\hat{Q}\frac{1}{\left(\omega-\hat{H}_0\right)}\hat{Q}=\hat{Q}\frac{1}{\left(\omega-\hat{H}_0\right)}=\frac{\hat{Q}}{\left(\omega-\hat{H}_0\right)}.
$$
With these definitions we can in turn define the wave function as
$$
\vert \Psi_0\rangle=\vert \Phi_0\rangle+\frac{\hat{Q}}{\omega-\hat{H}_0}\left(\omega-E+\hat{H}_I\right)\vert \Psi_0\rangle.
$$
This equation is again nothing but a formal rewrite of Schr\"odinger's equation
and does not represent a practical calculational scheme.
It is a non-linear equation in two unknown quantities, the energy \( E \) and the exact
wave function \( \vert \Psi_0\rangle \). We can however start with a guess for \( \vert \Psi_0\rangle \) on the right hand side of the last equation.
The most common choice is to start with the function which is expected to exhibit the largest overlap with the wave function we are searching after, namely \( \vert \Phi_0\rangle \). This can again be inserted in the solution for \( \vert \Psi_0\rangle \) in an iterative fashion and if we continue along these lines we end up with
$$
\vert \Psi_0\rangle=\sum_{i=0}^{\infty}\left\{\frac{\hat{Q}}{\omega-\hat{H}_0}\left(\omega-E+\hat{H}_I\right)\right\}^i\vert \Phi_0\rangle,
$$
for the wave function and
$$
\Delta E=\sum_{i=0}^{\infty}\langle \Phi_0\vert \hat{H}_I\left\{\frac{\hat{Q}}{\omega-\hat{H}_0}\left(\omega-E+\hat{H}_I\right)\right\}^i\vert \Phi_0\rangle,
$$
which is now a perturbative expansion of the exact energy in terms of the interaction
\( \hat{H}_I \) and the unperturbed wave function \( \vert \Psi_0\rangle \).
In our equations for \( \vert \Psi_0\rangle \) and \( \Delta E \) in terms of the unperturbed solutions \( \vert \Phi_i\rangle \) we have still an undetermined parameter \( \omega \) and a dependecy on the exact energy \( E \). Not much has been gained thus from a practical computational point of view.
In Brilluoin-Wigner perturbation theory it is customary to set \( \omega=E \). This results in the following perturbative expansion for the energy \( \Delta E \)
$$
\Delta E=\sum_{i=0}^{\infty}\langle \Phi_0\vert \hat{H}_I\left\{\frac{\hat{Q}}{\omega-\hat{H}_0}\left(\omega-E+\hat{H}_I\right)\right\}^i\vert \Phi_0\rangle=
$$
$$
\langle \Phi_0\vert \left(\hat{H}_I+\hat{H}_I\frac{\hat{Q}}{E-\hat{H}_0}\hat{H}_I+
\hat{H}_I\frac{\hat{Q}}{E-\hat{H}_0}\hat{H}_I\frac{\hat{Q}}{E-\hat{H}_0}\hat{H}_I+\dots\right)\vert \Phi_0\rangle.
$$
$$
\Delta E=\sum_{i=0}^{\infty}\langle \Phi_0\vert \hat{H}_I\left\{\frac{\hat{Q}}{\omega-\hat{H}_0}\left(\omega-E+\hat{H}_I\right)\right\}^i\vert \Phi_0\rangle=$$
$$
\langle \Phi_0\vert \left(\hat{H}_I+\hat{H}_I\frac{\hat{Q}}{E-\hat{H}_0}\hat{H}_I+
\hat{H}_I\frac{\hat{Q}}{E-\hat{H}_0}\hat{H}_I\frac{\hat{Q}}{E-\hat{H}_0}\hat{H}_I+\dots\right)\vert \Phi_0\rangle.
$$
This expression depends however on the exact energy \( E \) and is again not very convenient from a practical point of view. It can obviously be solved iteratively, by starting with a guess for \( E \) and then solve till some kind of self-consistency criterion has been reached.
Actually, the above expression is nothing but a rewrite again of the full Schr\"odinger equation.
Defining \( e=E-\hat{H}_0 \) and recalling that \( \hat{H}_0 \) commutes with \( \hat{Q} \) by construction and that \( \hat{Q} \) is an idempotent operator \( \hat{Q}^2=\hat{Q} \). Using this equation in the above expansion for \( \Delta E \) we can write the denominator
$$
\hat{Q}\frac{1}{\hat{e}-\hat{Q}\hat{H}_I\hat{Q}}=
$$
$$
\hat{Q}\left[\frac{1}{\hat{e}}+\frac{1}{\hat{e}}\hat{Q}\hat{H}_I\hat{Q}
\frac{1}{\hat{e}}+\frac{1}{\hat{e}}\hat{Q}\hat{H}_I\hat{Q}
\frac{1}{\hat{e}}\hat{Q}\hat{H}_I\hat{Q}\frac{1}{\hat{e}}+\dots\right]\hat{Q}.
$$
Inserted in the expression for \( \Delta E \) leads to
$$
\Delta E=
\langle \Phi_0\vert \hat{H}_I+\hat{H}_I\hat{Q}\frac{1}{E-\hat{H}_0-\hat{Q}\hat{H}_I\hat{Q}}\hat{Q}\hat{H}_I\vert \Phi_0\rangle.
$$
In RS perturbation theory we set \( \omega = W_0 \) and obtain the following expression for the energy difference
$$
\Delta E=\sum_{i=0}^{\infty}\langle \Phi_0\vert \hat{H}_I\left\{\frac{\hat{Q}}{W_0-\hat{H}_0}\left(\hat{H}_I-\Delta E\right)\right\}^i\vert \Phi_0\rangle=
$$
$$
\langle \Phi_0\vert \left(\hat{H}_I+\hat{H}_I\frac{\hat{Q}}{W_0-\hat{H}_0}(\hat{H}_I-\Delta E)+
\hat{H}_I\frac{\hat{Q}}{W_0-\hat{H}_0}(\hat{H}_I-\Delta E)\frac{\hat{Q}}{W_0-\hat{H}_0}(\hat{H}_I-\Delta E)+\dots\right)\vert \Phi_0\rangle.
$$
Recalling that \( \hat{Q} \) commutes with \( \hat{H_0} \) and since \( \Delta E \) is a constant we obtain that
$$
\hat{Q}\Delta E\vert \Phi_0\rangle = \hat{Q}\Delta E\vert \hat{Q}\Phi_0\rangle = 0.
$$
Inserting this results in the expression for the energy results in
$$
\Delta E=\langle \Phi_0\vert \left(\hat{H}_I+\hat{H}_I\frac{\hat{Q}}{W_0-\hat{H}_0}\hat{H}_I+
\hat{H}_I\frac{\hat{Q}}{W_0-\hat{H}_0}(\hat{H}_I-\Delta E)\frac{\hat{Q}}{W_0-\hat{H}_0}\hat{H}_I+\dots\right)\vert \Phi_0\rangle.
$$
We can now this expression in terms of a perturbative expression in terms of \( \hat{H}_I \) where we iterate the last expression in terms of \( \Delta E \)
$$
\Delta E=\sum_{i=1}^{\infty}\Delta E^{(i)}.
$$
We get the following expression for \( \Delta E^{(i)} \)
$$
\Delta E^{(1)}=\langle \Phi_0\vert \hat{H}_I\vert \Phi_0\rangle,
$$
which is just the contribution to first order in perturbation theory,
$$
\Delta E^{(2)}=\langle\Phi_0\vert \hat{H}_I\frac{\hat{Q}}{W_0-\hat{H}_0}\hat{H}_I\vert \Phi_0\rangle,
$$
which is the contribution to second order.
$$
\Delta E^{(3)}=\langle \Phi_0\vert \hat{H}_I\frac{\hat{Q}}{W_0-\hat{H}_0}\hat{H}_I\frac{\hat{Q}}{W_0-\hat{H}_0}\hat{H}_I\Phi_0\rangle-
\langle\Phi_0\vert \hat{H}_I\frac{\hat{Q}}{W_0-\hat{H}_0}\langle \Phi_0\vert \hat{H}_I\vert \Phi_0\rangle\frac{\hat{Q}}{W_0-\hat{H}_0}\hat{H}_I\vert \Phi_0\rangle,
$$
being the third-order contribution.
In the shell-model lectures we showed that we could rewrite the exact state function for say the ground state, as a linear expansion in terms of all possible Slater determinants. That is, we define the ansatz for the ground state as
$$
|\Phi_0\rangle = \left(\prod_{i\le F}\hat{a}_{i}^{\dagger}\right)|0\rangle,
$$
where the index \( i \) defines different single-particle states up to the Fermi level. We have assumed that we have \( N \) fermions.
A given one-particle-one-hole (\( 1p1h \)) state can be written as
$$
|\Phi_i^a\rangle = \hat{a}_{a}^{\dagger}\hat{a}_i|\Phi_0\rangle,
$$
while a \( 2p2h \) state can be written as
$$
|\Phi_{ij}^{ab}\rangle = \hat{a}_{a}^{\dagger}\hat{a}_{b}^{\dagger}\hat{a}_j\hat{a}_i|\Phi_0\rangle,
$$
and a general \( ApAh \) state as
$$
|\Phi_{ijk\dots}^{abc\dots}\rangle = \hat{a}_{a}^{\dagger}\hat{a}_{b}^{\dagger}\hat{a}_{c}^{\dagger}\dots\hat{a}_k\hat{a}_j\hat{a}_i|\Phi_0\rangle.
$$
We use letters \( ijkl\dots \) for states below the Fermi level and \( abcd\dots \) for states above the Fermi level. A general single-particle state is given by letters \( pqrs\dots \).
We can then expand our exact state function for the ground state as
$$
|\Psi_0\rangle=C_0|\Phi_0\rangle+\sum_{ai}C_i^a|\Phi_i^a\rangle+\sum_{abij}C_{ij}^{ab}|\Phi_{ij}^{ab}\rangle+\dots
=(C_0+\hat{C})|\Phi_0\rangle,
$$
where we have introduced the so-called correlation operator
$$
\hat{C}=\sum_{ai}C_i^a\hat{a}_{a}^{\dagger}\hat{a}_i +\sum_{abij}C_{ij}^{ab}\hat{a}_{a}^{\dagger}\hat{a}_{b}^{\dagger}\hat{a}_j\hat{a}_i+\dots
$$
Since the normalization of \( \Psi_0 \) is at our disposal and since \( C_0 \) is by hypothesis non-zero, we may arbitrarily set \( C_0=1 \) with
corresponding proportional changes in all other coefficients. Using this so-called intermediate normalization we have
$$
\langle \Psi_0 | \Phi_0 \rangle = \langle \Phi_0 | \Phi_0 \rangle = 1,
$$
resulting in
$$
|\Psi_0\rangle=(1+\hat{C})|\Phi_0\rangle.
$$
In a shell-model calculation, the unknown coefficients in \( \hat{C} \) are the eigenvectors which result from the diagonalization of the Hamiltonian matrix.
How can we use perturbation theory to determine the same coefficients? Let us study the contributions to second order in the interaction, namely
$$
\Delta E^{(2)}=\langle\Phi_0\vert \hat{H}_I\frac{\hat{Q}}{W_0-\hat{H}_0}\hat{H}_I\vert \Phi_0\rangle.
$$
The intermediate states given by \( \hat{Q} \) can at most be of a \( 2p-2h \) nature if we have a two-body Hamiltonian. This means that second order in the perturbation theory can have \( 1p-1h \) and \( 2p-2h \) at most as intermediate states. When we diagonalize, these contributions are included to infinite order. This means that higher-orders in perturbation theory bring in more complicated correlations.
If we limit the attention to a Hartree-Fock basis, then we have that \( \langle\Phi_0\vert \hat{H}_I \vert 2p-2h\rangle \) is the only contribution and the contribution to the energy reduces to
$$
\Delta E^{(2)}=\frac{1}{4}\sum_{abij}\langle ij\vert \hat{v}\vert ab\rangle \frac{\langle ab\vert \hat{v}\vert ij\rangle}{\epsilon_i+\epsilon_j-\epsilon_a-\epsilon_b}.
$$
If we compare this to the correlation energy obtained from full configuration interaction theory with a Hartree-Fock basis, we found that
$$
E-E_0 =\Delta E=
\sum_{abij}\langle ij | \hat{v}| ab \rangle C_{ij}^{ab},
$$
where the energy \( E_0 \) is the reference energy and \( \Delta E \) defines the so-called correlation energy.
We see that if we set
$$
C_{ij}^{ab} =\frac{1}{4}\frac{\langle ab \vert \hat{v} \vert ij \rangle}{\epsilon_i+\epsilon_j-\epsilon_a-\epsilon_b},
$$
we have a perfect agreement between FCI and MBPT. However, FCI includes such \( 2p-2h \) correlations to infinite order. In order to make a meaningful comparison we would at least need to sum such correlations to infinite order in perturbation theory.
Summing up, we can see that


Get all available regions for the AWS Cloudtrail service.
| Return type: | list |
|---|---|
| Returns: | A list of boto.regioninfo.RegionInfo |
AWS Cloud Trail This is the CloudTrail API Reference. It provides descriptions of actions, data types, common parameters, and common errors for CloudTrail.
CloudTrail is a web service that records AWS API calls for your AWS account and delivers log files to an Amazon S3 bucket. The recorded information includes the identity of the user, the start time of the AWS API call, the source IP address, the request parameters, and the response elements returned by the service.
As an alternative to using the API, you can use one of the AWS SDKs, which consist of libraries and sample code for various programming languages and platforms (Java, Ruby, .NET, iOS, Android, etc.). The SDKs provide a convenient way to create programmatic access to AWSCloudTrail. For example, the SDKs take care of cryptographically signing requests, managing errors, and retrying requests automatically. For information about the AWS SDKs, including how to download and install them, see the `Tools for Amazon Web Services page`_.
See the CloudTrail User Guide for information about the data that is included with each AWS API call listed in the log files.
alias of JSONResponseError
From the command line, use create-subscription.
Creates a trail that specifies the settings for delivery of log data to an Amazon S3 bucket.
Support for passing Trail as a parameter ends as early as February 25, 2014. The request and response examples in this topic show the use of parameters as well as a Trail object. Until Trail is removed, you can use either Trail or the parameter list.
| Parameters: |
|
|---|
Retrieves the settings for some or all trails associated with an account.
| Parameters: | trail_name_list (list) – The list of trails. |
|---|
Returns a JSON-formatted list of information about the specified trail. Fields include information on delivery errors, Amazon SNS and Amazon S3 errors, and start and stop logging times for each trail.
The CloudTrail API is currently undergoing revision. This action currently returns both new fields and fields slated for removal from the API. The following lists indicate the plans for each field:
List of Members Planned for Ongoing Support
List of Members Scheduled for Removal
No replacements have been created for LatestDeliveryAttemptSucceeded and LatestNotificationAttemptSucceeded . Use LatestDeliveryError and LatestNotificationError to evaluate success or failure of log delivery or notification. Empty values returned for these fields indicate success. An error in LatestDeliveryError generally indicates either a missing bucket or insufficient permissions to write to the bucket. Similarly, an error in LatestNotificationError indicates either a missing topic or insufficient permissions.
| Parameters: | name (string) – The name of the trail for which you are requesting the current status. |
|---|
Starts the recording of AWS API calls and log file delivery for a trail.
| Parameters: | name (string) – The name of the trail for which CloudTrail logs AWS API calls. |
|---|
Suspends the recording of AWS API calls and log file delivery for the specified trail. Under most circumstances, there is no need to use this action. You can update a trail without stopping it first. This action is the only way to stop recording.
| Parameters: | name (string) – Communicates to CloudTrail the name of the trail for which to stop logging AWS API calls. |
|---|
From the command line, use update-subscription.
Updates the settings that specify delivery of log files. Changes to a trail do not require stopping the CloudTrail service. Use this action to designate an existing bucket for log delivery. If the existing bucket has previously been a target for CloudTrail log files, an IAM policy exists for the bucket.
Support for passing Trail as a parameter ends as early as February 25, 2014. The request and response examples in this topic show the use of parameters as well as a Trail object. Until Trail is removed, you can use either Trail or the parameter list.
| Parameters: |
|
|---|
Exceptions that are specific to the cloudtrail module.
Raised when the S3 bucket does not allow Cloudtrail to write files into the prefix.
Raised when the SNS topic does not allow Cloudtrail to post messages.
Raised when there was an internal Cloudtrail error.
Raised when an invalid S3 bucket name is passed to Cloudtrail.
Raised when an invalid key prefix is given.
Raised when an invalid SNS topic name is passed to Cloudtrail.
Raised when the trail name is invalid.
Raised when no more trails can be created.
Raised when the given S3 bucket does not exist.
Raised when the given trail name already exists.
Raised when the given trail name is not found.
Raised when no trail name was provided.


Company will pay person $3K per month to review marijuana
by CNN NewsourceThis could be a highly sought-after job.
A company wants to pay someone to review marijuana products.
American Marijuana is a medical marijuana online magazine that provides research on cannabis products.
The company is looking for someone to receive and critique a box containing different products every month. The products can range from weed, vapes, edibles, and CBD oils.
But you have to live somewhere in the U.S. or Canada where medical marijuana is legal. The candidate must also critique the cannabis on camera and post blogs about the products.
Along with receiving free cannabis products, the person will be paid up to $3,000 a month or a $36,000 a year salary.
You can learn more about the opportunity and apply on their website .


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In a period of 18yrs I've been through eight schools, In addition I've learnt in two diffrent curriculums. At the momment i currently have two certificates; one being my:
First and foremost
I've always been fascinated by programming, ever since I glanced on a monitor
displaying code someone was working on.
All along highschool,
I was certain I needed to do something in
the lines of information technology.
It's not until my fourth year of high school that I realized I was to
major in programming.
This project is an application where users can create quotes and have those quotes voted on whether they are terrible or are inspirational.
infoTypeScript
My own a pizza place as a way of trying to widen my overall customer base, I decided to create a web application where my customers order different sizes of pizzas with one or more toppings.
infoJavaScript


Artsem
Home
About Me
Welcome To My Artsem Holdvekht Web Site
Linked In
My LinkedIn Profile.
View details »
GitHub
You can access my repositoy here.
View details »


{% load i18n %} {% block subject %} {% blocktrans %}{{ site_name }} - Workflow run '{{ name }}'' has finished!{% endblocktrans %} {% endblock %} {% block html_body %}
{% trans "A workflow run you started has finished!" %}
| {% trans "Name" %} | {{ name }} |
|---|---|
| {% trans "Description" %} | {{ description }} |


Lisa has completed Wyncode Academy's Accelerated Learning Program as Full Stack Web Developer. The purpose of Accelerated Learning is to fast-track ambitious and driven people with the right mindset into a new career.
The course constantly revolves around contemporary projects relevant to the industry. As a result of this, the learning process is extremely effective as well as relevant to most companies' tasks.
Examination Project.
A web aplication that helps you calculate and remember what to pack on your travels.
Click image to paly demo
Close Project


Two men arrested at huge cannabis factory in Wednesbury
Two men have been charged after police raided a huge cannabis factory in Wednesbury containing 417 plants.
by Jamie BrassingtonThe haul was uncovered at an address on Hollies Drive on Thursday.
West Midlands Police arrested Klodian Ndoca, aged 31, and Arjan Nikollaj, 25, inside the property.
They appeared at Walsall Magistrates Court on Friday, charged with the production of cannabis.
The force values the average of cannabis plants at £1,000 each, however the value of this cannabis find is not yet known.
The plants were discovered across seven large rooms and a loft space.
A photograph, released by police, showed dozens of cannabis plants growing under artificial lights inside the building.
Wednesbury's police team tweeted: "Officers from @WednesburyWMP conducted a drugs warrant on a premises on Hollies Drive Wednesbury and uncovered 7 large rooms and a loft space was being used to cultivate cannabis. 2 suspects were arrested from the property and a total of 417 plants seized @CannabisTeamWMP"


Attribute
public enum Attribute : Int, CaseIterable
JSONFormat
attributes that can be output.
See also
JSONFormat
for usage.
-
Output the timestamp as an
Int
.Declaration
Swift
case timestamp
-
Output the level as a
String
such as ERROR, WARNING, INFO, etc.Declaration
Swift
case level
-
Output the tag field as a
String
.Declaration
Swift
case tag
-
Output the message field as a
String
.Declaration
Swift
case message
-
Output the processName field as a
String
.Declaration
Swift
case processName
-
Output the processIdentifier field as a
Int
.Declaration
Swift
case processIdentifier
-
Output the threadIdentifier field as a
UInt64
.Declaration
Swift
case threadIdentifier
-
Output the file field as a
String
.Declaration
Swift
case file
-
Output the function field as a
String
.Declaration
Swift
case function
-
Output the line field as a
Int
.Declaration
Swift
case line


{% extends 'global/base.html' %} {% load i18n static %} {% block content %}
{% trans "We’re delighted to welcome you as a part of Django Girls family! We’ve deployed your event’s website now and an information pack with access details is on the way to your inbox right now." %}
{% trans "In the information pack, you will receive access to the following:" %}
{% trans "We hope you’re as excited as we are about starting this adventure!" %}
{% blocktrans %}Good luck and see you on Slack 👋
Django Girls Team{% endblocktrans %}


Call _transform() if you want to use single CPU with all samples
if X is None or self.cols is None:
raise AttributeError("None data or feature input")
self.X = X
self.data_lines = len(X)
if self.max_sample == 0 and self.max_process == 1:
// then make sure that it is the right size
if X.shape[1] != self._dim:
raise ValueError("Unexpected input dimension %d, expected %d" % (X.shape[1], self._dim, ))
if not self.cols:
return X


| Table 1 |
Highest projected exposure results for all models, scenarios ... |
| Table 2 |
Interpretation of ACCVI results |
| Table 3 |
Highest projected vulnerability results for all models, scen ... |
| Table 4 |
Increment percentage/anomalies results for all models, scena ... |