| Methods' Details |
getProgrammaticFuntionName
| string |
| getProgrammaticFuntionName( |
[in] string |
aDisplayName ); |
- Description
- returns the internal function name for an user-visible name.
The user-visible name of a function is the name shown to the
user. It may be translated to the current language of the AddIn,
so it is never stored in files. It should be a single word and is
used when entering or displaying formulas.
Attention: The method name contains a spelling error. Due to
compatibility reasons the name cannot be changed.
- Parameter aDisplayName
- the user-visible name of a function.
- Returns
- the exact name of the method within its interface.
|
|
getDisplayFunctionName
| string |
| getDisplayFunctionName( |
[in] string |
aProgrammaticName ); |
- Description
- returns the user-visible function name for an internal name.
The user-visible name of a function is the name shown to the
user. It may be translated to the current language of the AddIn,
so it is never stored in files. It should be a single word and is
used when entering or displaying formulas.
- Parameter aProgrammaticName
- is the exact name of a method within its interface.
- Returns
- the user-visible name of the specified function.
|
|
getFunctionDescription
| string |
| getFunctionDescription( |
[in] string |
aProgrammaticName ); |
- Description
- returns the description of a function.
The description is shown to the user when selecting functions.
It may be translated to the current language of the AddIn.
- Parameter aProgrammaticName
- is the exact name of a method within its interface.
- Returns
- the description of the specified function.
|
|
getDisplayArgumentName
| string |
| getDisplayArgumentName( |
[in] string |
aProgrammaticFunctionName, |
| [in] long |
nArgument ); |
- Description
- returns the user-visible name of the specified argument.
The argument name is shown to the user when prompting for
arguments. It should be a single word and may be translated
to the current language of the AddIn.
- Parameter aProgrammaticFunctionName
- is the exact name of a method within its interface.
- Parameter nArgument
- the index of the argument (0-based).
- Returns
- the user-visible name of the specified argument.
|
|
getArgumentDescription
| string |
| getArgumentDescription( |
[in] string |
aProgrammaticFunctionName, |
| [in] long |
nArgument ); |
- Description
- returns the description of the specified argument.
The argument description is shown to the user when prompting
for arguments. It may be translated to the current language of
the AddIn.
- Parameter aProgrammaticFunctionName
- is the exact name of a method within its interface.
- Parameter nArgument
- the index of the argument (0-based).
- Returns
- the description of the specified argument.
|
|
getProgrammaticCategoryName
| string |
| getProgrammaticCategoryName( |
[in] string |
aProgrammaticFunctionName ); |
- Description
- returns the programmatic name of the category the function
belongs to.
The category name is used to group similar functions together.
The programmatic category name should always be in English, it is
never shown to the user.
It should be one of the following names if the function falls into
the corresponding category.
- Database
- for functions that operate with data organized in tabular form
like databases.
- Date&Time
- for functions that deal with date or time values.
- Financial
- for functions that solve financial problems.
- Information
- for functions that provide information about cells.
- Logical
- for functions that deal with logical expressions.
- Mathematical
- for mathematical functions.
- Matrix
- for matrix functions.
- Statistical
- for statistical functions.
- Spreadsheet
- for functions that deal with cell ranges.
- Text
- for functions that deal with text strings.
- Add-In
- for additional functions.
- Parameter aProgrammaticFunctionName
- is the exact name of a method within its interface.
- Returns
- the category name the specified function belongs to.
|
|
getDisplayCategoryName
| string |
| getDisplayCategoryName( |
[in] string |
aProgrammaticFunctionName ); |
- Description
- returns the user-visible name of the category the function
belongs to.
This is used when category names are shown to the user.
- Parameter aProgrammaticFunctionName
- is the exact name of a method within its interface.
- Returns
- the user-visible category name the specified function
belongs to.
|
|
Copyright © 2013, The Apache Software Foundation, Licensed under the Apache License, Version 2.0. Apache, the Apache feather logo, Apache OpenOffice and OpenOffice.org are trademarks of The Apache Software Foundation. Other names may be trademarks of their respective owners.


NSColor
public extension NSColor
Extension for NSColor
to support colorset files.
-
Gets a color from the shared
ColorSet
instance.This methods will return the correct color, depending on the current user interface mode.
If the requested color is found and has a dark mode variant, and if dark mode is on, the variant will be returned instead of the main color.For this reason, you should never store color objects returned by this method, but instead ask for the color each time you need it (eg. in drawing code).
This is because the user interface mode may change while the application is running. As all views will be redrawned, this is to ensure the correct color is used.Lightness variants may be requested by adding a
.
(dot) and a lightness value from0
to100
in the name, such asSomeColor.75
.
This will return the base color, with the lightness changed to 75%.
Note that the lightness will be automatically reversed in dark mode (if the lightness value coresponds to a predefined lightness pair, the corresponding lightness will be used.It’s also possible to refer to lightness variants using names, if custom names were added, such as
SomeColor.SomeVariant
.Standard Cocoa colors can also be retrieved using the
NS
prefix, such asNSSecondaryLabelColor
forNSColor.secondaryLabelColor
.Declaration
Swift
@objc class func from(colorSet name: String) -> NSColor?
Parameters
name
The name of the color to retrieve.
Return Value
The color object, if found.
-
Creates a color from
HSL
components.Note that the
HSL
values will be converted toRGB
.
The color object will be created usingsRGB
values.Declaration
Swift
@objc convenience init(hue: CGFloat, saturation: CGFloat, lightness: CGFloat, alpha: CGFloat)
Parameters
hue
The hue component -
0
to1
.saturation
The saturation component -
0
to1
.lightness
The lightness component -
0
to1
.alpha
The alpha component -
0
to1
. -
Finds the best text color for a specific background color, to ensure a good contrast ration between the text and the background color.
Note that the returned text color will either be black or white, depending on the background color.
Declaration
Swift
@objc class func bestTextColorForBackgroundColor(_ background: NSColor) -> NSColor
Parameters
background
The background color
Return Value
A suitable text color for the background color.
-
Finds the best text color for a specific background color, to ensure a good contrast ration between the text and the background color.
The caller is responsible for passing two alternative text colors.
The light one will be choosen on dark backgrounds, while the dark one will be chosen on light backgrounds.In order to ensure a good contrast ratio, these two colors should be close to black and white.
Declaration
Swift
@objc class func bestTextColorForBackgroundColor(_ background: NSColor, lightTextColor: NSColor, darkTextColor: NSColor) -> NSColor
Parameters
background
The background color
lightTextColor
The light text color (for use on dark backgrounds).
darkTextColor
The dark text color (for use on light backgrounds).
Return Value
Depending on the background color, either the
lightTextColor
or thedarkTextColor
parameter. -
Gets the color as an RGB hexadecimal string, prefixed with
#
.Declaration
Swift
@objc var hexString: String { get }
-
Gets the
HSL
components of the color.Declaration
Swift
@objc func getHue(_ hue: UnsafeMutablePointer<CGFloat>?, saturation: UnsafeMutablePointer<CGFloat>?, lightness: UnsafeMutablePointer<CGFloat>?, alpha: UnsafeMutablePointer<CGFloat>?)
Parameters
hue
Upon return, contains the hue component of the color object -
0
to1
.saturation
Upon return, contains the saturation component of the color object -
0
to1
.lightness
Upon return, contains the lightness component of the color object -
0
to1
.alpha
Upon return, contains the alphas component of the color object -
0
to1
. -
Gets the
RGB
components of the color as a tuple.Declaration
Swift
@nonobjc func rgb() -> (red: CGFloat, green: CGFloat, blue: CGFloat, alpha: CGFloat)
Return Value
A tuple with the
RGB
components. -
Gets the
HSB
components of the color as a tuple.Declaration
Swift
@nonobjc func hsb() -> (hue: CGFloat, saturation: CGFloat, brightness: CGFloat, alpha: CGFloat)
Return Value
A tuple with the
HSB
components. -
Gets the
HSL
components of the color as a tuple.Declaration
Swift
@nonobjc func hsl() -> (hue: CGFloat, saturation: CGFloat, lightness: CGFloat, alpha: CGFloat)
Return Value
A tuple with the
HSL
components. -
Creates a new color by modifying the hue components of the
HSL
representation.Declaration
Swift
@objc func byChangingHue(_ h: CGFloat) -> NSColor
Return Value
The new color
-
Creates a new color by modifying the saturation components of the
HSL
representation.Declaration
Swift
@objc func byChangingSaturation(_ s: CGFloat) -> NSColor
Return Value
The new color
-
Creates a new color by modifying the lightness components of the
HSL
representation.Declaration
Swift
@objc func byChangingLightness(_ l: CGFloat) -> NSColor
Return Value
The new color


Up on the white veranda, she wears a necktie and a Panama hat,
Her passport shows a face from another time and place, she looks a-nothing like that,
And all of the remnants of her recent past are scattered in the wild wind.
She walks across the marble floor where a voice from the gambling room is calling her to come on in,
She smiles, walks the other way
As the last ship sails and the moon fades away from Black Diamond Bay.
As the morning light breaks open, the Greek comes down and he asks for rope and a pen that will write.
"Pardon, monsieur," the desk clerk says, carefully removes his fez, "am I hearing you right?"
And, as the yellow fog is lifting, the Greek is quickly heading for the second floor,
She passes him on the spiral staircase, thinking he's the Soviet Ambassador.
She starts to speak, but he walks away
As the storm clouds rise and the palm branches sway on Black Diamond Bay.

The desk clerk heard the woman laugh as he looked around in the aftermath and the soldier got tough,
He tried to grab the woman's hand, said, "Here's a ring, it cost a grand!" She said, "That ain't enough."
Then she ran upstairs to pack her bags while a horse-drawn taxi waited at the curb,
She passed the door where the Greek had locked where a handwritten sign read a-"Do Not Disturb".
She knocked upon it anyway
As the sun went down and the music did play on Black Diamond Bay.
"I've got to talk to someone quick!" But the Greek said, "Go away!", and he kicked the chair to the floor.
He hung there from the chandelier, she cried, "Help, there's danger near, please a-open up a-the door!"
Then the volcano erupted and the lava flowed down from the mountain high above,
The soldier and the tiny man were crouched in the corner thinking of forbidden love,
The desk clerk said, "It happens every day",
As the stars fell down and the moons fade away
2 on Black Diamond Bay.
As the island slowly sank, the loser finally broke the bank in the gambling room.
The dealer said, "It's too late now, you can take your money, but I don't know how you'll spend it in the tomb."
The tiny man bit the soldier's ear as the floor caved in and the boiler in the basement blew,
While she's out on the balcony where a stranger tells her, "My darling, je vous aime beaucoup."
3
She sheds a tear and then begins to pray
As the sun burns on and the smoke drifts away from Black Diamond Bay.
I was sitting home alone one night in L.A., watching old Cronkite on the seven o'clock news,
It seems there was an earthquake that left nothing but a Panama hat and a pair of old Greek shoes.
It didn't seem like much was happening, so I turned it off and went to grab another beer,
Seem like every time you turn around there's another hard-luck story that you're gonna hear
And there's really nothing anyone can say –
And I never did plan to go anyway to Black Diamond Bay.
1
Translation of the French: "Wait, please".
2
Other lyrics sources present an alternate (but obviously incorrect) lyric here: "As the starts fell down and the fields burned away".
3
Translation of the French: "I love you a lot". This is a reference to a popular song written by Anna Sosenko in 1935 called "Darling, Je Vous Aime Beaucoup", which, although grammatically correct, is a deliberate attempt at bad French.


Product Usage
Describe how your company uses this product. What business issues does it address? Which part of your company uses it?* (100 character minimum)
characters used
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I use the product
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What is your level of experience with this product?*
Please choose an option from the list
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How many working hours does this product save you?*
Where did you use this product?*
Currently use this product
In a different role at my current company
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What was the industry of the company where you used this product?*
Please select an industry
Accounting
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Support


About
UI/UX Designer
Hello there! I am a UI/UX Designer and I have been designing websites and mobile applications for more than two years.
Besides designing, I like to explore new things and travelling new different places and love watching movies and listening to music.
Skills
HTML5 90%
CSS3 90%
JavaScript 75%
Bootstrap 80%
Photoshop 90%
Illustrator 55%
Resume
Summary
Tika B.K.
Innovative and deadline-driven Designer with 2+ years of experience in app and web designing.
- Manbhawan, Lalitpur, Nepal
-<EMAIL_ADDRESS>Education
Bachelors in Computer Engineering
2011 - 2015
Kantipur Engineering College, Dhapakhel, Lalitpur
Professional Experience
UI/UX Designer
2019 - Present
View9, Sankhamul, Kathmandu
UI/UX Designer
2018 - 2019
Neptsoft Pvt. Ltd., Arubari, Kathmandu
Web Designer Intern
2018
OnlineZeal, Tinkune, Kathmandu


Class It Up
Ruby's Classes
11/30/15
When I first learned about classes, it was a heady concept to wrap my head around. Classes create objects that have specific methods and variables? Huh? (Let alone the fact that I didn't really grasp what a method or a variable was in the first place. Or the fact that a method is really just a class-based function.)
But I digress! Classes and objects. A class is like a template, and objects are the actual occurence/creation of that template. For example, let's say I wanted to make an RPG crime noir text based Ruby console game. (Inspiration from Learn Ruby the Hard Way, Exercise 43.) And let's say I wanted to have a character, a detective. As such, I could write it like this:
class Detective def initialize(name) @@weapon = ["knife", "gun", "cigarettes"] @name = name end def tell_me_about_yourself puts "My name is Detective #{name}, and I fight the crime lords and underlings of this rotten city." puts "I have a #{print_weapon_list}." end def add_weapon(weapon) @@weapon.push(weapon) end def print_weapon_list count = 0 while count < @@weapon.length - 2 print @@weapon[0] + ", " count += 1 end print "and" +<EMAIL_ADDRESS>end end a_detective = Detective.new("Detective Bronson")
So essentially this code is creating a new detective object. You can pass in a name for your detective character through the initialize method. The initialize method creates a set of instance variables (variables which can be used across all instances of this particular class, as opposed to a local variable which can be used in a particular method).
The detective class comes with a few other fun tricks - you can add weapons to the detective's arsenal through the add_weapon methods, and you can get some info on your detective, through the tell_me_about_yourself method. That particular method calls another method to help it out with printing the list of weapons the detective currently owns.
All in all, classes are fun because they all for more interesting relationships between data and methods. Meanwhile, I will happily continue sleuthing out better ways to use them!


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A MIDSUMMER NIGHTS DREAM Cast: Kevin Kline, Michelle Pfeiffer, Rupert Everett, Stanley Tucci, Calista Flockhart, Anna Friel, Dominic West, Christian Bale, David Strathairn, Sophie Marceau Director: Michael Hoffman Screenplay: Michael Hoffman, based on the play by William Shakespeare Reviewed by Luke Buckmaster
On the Buckmaster scale of 0 stars (bomb), to 5 stars (a masterpiece): 3 stars
Whilst A Midsummer Night's Dream may not be one of Shakespeare's best plays, it's arguably his most atmospheric. Only one previous film adaptation has been made by a major studio, and that was in the 1930's. The reason: it's such a big ask for a motion picture. The Bard intended his play to be a magical and luminous experience, and these are qualities that can't be produced through just a script. Thankfully, filmmaker Michael Hoffman's take on the well-known production is pleasing to the senses, and with the aid of cinematographer Oliver Stapleton (One Fine Day), he has created quite a spectacular mythical world. The lively visual energy of A Midsummer Night's Dream is its selling point both commercially and artistically and it evokes, as Shakespeare would have would intended, a sense of wonder and magic. Although some of the film's other elements bring it down - which, incidentally, are mostly the same things that limited the play's narrative success - this piece will please the masses, and for all the right reasons.
Instead of 16th century Greece the setting is 19th century Tuscany, and the bicycle has just been invented. Kevin Kline is Nick Bottom, a comical, obnoxious but courageous actor who is assigned to play Pyramus in 'Pyramus and Thisby,' an absurd drama from a company of struggling entertainers.  Meanwhile, four star-crossed lovers are pursuing each other in a magical forest. Helena (Calista Flockhart) loves Demetrius (Christian Bale), who barely acknowledges her existence and is engaged to marry Hermia (Christian Bale), but Hermia's true object of affection is Lysander (Dominic West). The Fairy King Oberon (Rupert Everett) watches them from a distance, and instructs his mischievous servant Puck (Stanley Tucci) to find a special kind of flower juice. A drop of this juice, once placed on the eyelids of somebody sleeping, will make them fall instantly in love to the first person they see upon waking. Puck, of course, worsens the situation by placing the juice on the wrong set of eyelids.
Given the nature of his material, Hoffman's direction is quite heavy handed. Much of the cast, too, try a little too hard to make it all work. Kevin Kline is the only lead performer who looks completely natural on the screen, and almost effortlessly entertains. Bottom, as a comical character, is one of Shakespeare's finest, and Kline fits the criteria perfectly. Calista "Ally McBeal" Flockhart, on the other hand, is more unconventional in her approach to Helena's eccentric personality. Flockhart overplays her somewhat, obviously intending to portray love-struck Shakespearean craziness, but she misfires somewhere along the line. Perhaps it's because she is the only actor who looks like she's been dragged from the set of Ally McBeal and asked to read Shakespeare. Flockhart, and especially Hoffman, are two production members who sometimes make A Midsummer Night's Dream feel like it is taking itself a little too seriously. Even in the final scene, in which Puck recites his famous speech ("if we shadows have offended, think but this, and all is mended…"), Hoffman misses the point entirely. He takes the speech very seriously, whereas Shakespeare intended it to ask forgiveness for those who were hoping for another Macbeth or Hamlet.
Be that as it may, A Midsummer Nigh'ts Dream is a solid and entertaining adaptation with some nice touches, both visually and literately. Watching cast members wizz around on bicycles is a novel idea, as are a couple of fun scenes that audiences will get a hoot from, including a good old fashioned female mud fight and, as Geoffrey Rush in Shakespeare in Love voiced, a "bit with a dog." The film's narrative structure, like the play's, is simplistic if not a little trite, but it was never intended to be something profound. A Midsummer Night's Dream is probably the closest description of Melrose Place in the 16th century (or, as it is here, the 19th century) that one can find. If you are tossing up whether to see Michael Hoffman's beautifully textured, visually entrancing and charming film or wait for the next high school production, I know which one I'd choose.
Read more of my reviews at In Film Australia http://infilmau.iah.net
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We had the chance to meet the Muséee Picasso Paris with Gobelins, and they gave us the brief for their new mobile application. As the museum is reopening in fall 2014, they needed a way to communicate about the national event, not only inside the museum, but an mobile application that can be experienced everywhere, every time. We worked during 3 month to find a idea, design it and produce it. Our though was : Discover the Pablo Picasso Universe. The user can browse trough constellations, the immensity of his work. That leaded to the black and white layout with the dots.
Team : Alexia Dupré-Doàn (Design) – Louis Ansa (Design) – Christophe Massolin (Development) – Kolin Weidmann (Development)


{{ define "main" }}
This is an index of all commands in rclone. Run rclone command --help to see the help for that command.
rclone command --help


--- layout: post title: ! 'Top Tip: Restrict Dimensions Requests to Prime Only' tags: - Serena Dimensions - Software Configuration Management status: publish type: post published: true meta: _edit_last: '451289' --- If you are a Serena Dimensions administrator you might find this of some use, otherwise I'm afraid it's 'move along, nothing to see here...' Let's explain the background: Dimensions supports the the concept of a Primed request (or change document in pre rel 10 terminology), another name for this is 'based on'. The idea is that you create a parent request type (e.g. a Request For Change -- RFC) and child request type (e.g. Development Request -- DR). The model would be that after an RFC is approved and sent to the development team for building. The development team then create one or more development requests to fulfil the requirements of the RFC. Dimensions further enhances this by allowing the administrator to define field mappings (priming) between parent and child requests. So for instance, when the user primes a new DR from an RFC it would be possible to copy over the short description and work order number (externally generated) to the DR However if is still possible to use the create new Request function to create a new DR manually. Usually this type of flexibility is desirable and all is good with the world. But sometimes our process restricts us so that we shouldn't allow a request to be generated unless it's based on a parent. A recent example I implemented was a RetroFit request, obviously a retrofit does not make sense unless it's part of a larger DR, although the retrofit could occur at any time and be carried out by a different developer. Dimensions itself has no specific feature to restrict this, you can achieve the same affect using mandatory user attributes. Although the effect it's perhaps not that elegant it does work. Now the implementation details


|
Excimontec
v1.0.0
An open-source KMC simulation software package for modeling the optoelectronic processes in organic semiconductor materials and devices, such as OPVs, OLEDs, and more.
|
This class extends the KMC_Lattice::Parameters_Simulation class to create a parameters object that holds all input parameters needed by a simulation. More...
#include <Parameters.h>
Inherits KMC_Lattice::Parameters_Simulation.
Public Member Functions | |
| bool | checkParameters () const |
| Checks the validity of the current parameter values. More... | |
| bool | importParameters (std::ifstream &inputfile) |
| Imports the values for all parameters by parsing the input filestream. More... | |
| Public Member Functions inherited from KMC_Lattice::Parameters_Simulation | |
| virtual | ~Parameters_Simulation () |
| Default virtual destructor. More... | |
| Parameters_Simulation () | |
| Default constructor that creates an empty object. More... | |
| bool | checkParameters () const |
| Checks the validity of the parameter member variables return true if the member variable parameters are valid return false if the member variable parameters are invalid. More... | |
Public Attributes | |
| bool | Enable_import_morphology_single = false |
| Specifies whether or not to import a single morphology file and use it on all processors. More... | |
| bool | Enable_import_morphology_set = false |
| Specifies whether or not to import a set of morphologies to be assigned to different processors. More... | |
| std::string | Morphology_set_format = "" |
| Defines the morphology set naming format. The standard naming format is morphology_#.txt where # is a wildcard for different numbers. More... | |
| int | N_test_morphologies = 0 |
| Defines the number of morphologies to be tested from the set. More... | |
| int | N_morphology_set_size = 0 |
| Defines the number of morphologies in the set. It is assumed that morphologies in the set are number from 0 to N_morphology_set_size-1. More... | |
| bool | Enable_extraction_map_output = false |
| Specifies whether or not extraction map data should be output to text file at the end of the simulation. More... | |
| double | Internal_potential |
| Defines the internal electrical potential across the semiconductor layer. More... | |
| bool | Enable_neat |
| Specifies whether or not to use a neat single phase material device architecture. A neat material morphology uses the donor material properties. More... | |
| bool | Enable_bilayer |
| Specifies whether or not to use a bilayer device architecture. More... | |
| int | Thickness_donor |
| Defines the donor layer thickness in number of sites when using bilayer architecture. More... | |
| int | Thickness_acceptor |
| Defines the acceptor layer thickness in number of sites when using bilayer architecture. More... | |
| bool | Enable_random_blend |
| Specifies whether or not to use a random blend material device architecture. More... | |
| double | Acceptor_conc |
| Defines the acceptor site volume concentration when using the random blend device architecture. More... | |
| bool | Enable_import_morphology |
| Specifies whether or not an imported morphology is being used to define the device architecture. More... | |
| std::string | Morphology_filename |
| The name of the morphology file to be imported. More... | |
| int | N_tests |
| Used as a generic counter for determining when a given simulation test is completed. More... | |
| bool | Enable_exciton_diffusion_test |
| Specifies whether or not the exciton diffusion test is to be run. More... | |
| bool | Enable_ToF_test |
| Specifies whether or not to run the time-of-flight charge transport test. More... | |
| bool | ToF_polaron_type |
| Specifies the type of polaron to test when performing the time-of-flight charge transport test. (false for electron and true for hole) More... | |
| int | ToF_initial_polarons |
| Defines the number of initial polarons to place in the simulation for the time-of-flight charge transport test. More... | |
| bool | Enable_ToF_random_placement |
| Specifies whether or not to use the random placement method for creating the initial polarons in the time-of-flight charge transport test. More... | |
| bool | Enable_ToF_energy_placement |
| Specifies whether or not to use the energy placement method for creating the initial polarons in the time-of-flight charge transport test. More... | |
| double | ToF_placement_energy |
| Defines the preferred energy within the DOS for initial polaron placement when using the energy placement method with the time-of-flight charge transport test. More... | |
| double | ToF_transient_start |
| Defines the start time of the transient data collected during the time-of-flight charge transport test. More... | |
| double | ToF_transient_end |
| Defines the end time of the transient data collected during the time-of-flight charge transport test. More... | |
| int | ToF_pnts_per_decade |
| Defines the collected transient data time resolution in number of points per decade for the time-of-flight charge transport test. More... | |
| bool | Enable_IQE_test |
| Specifies whether or not to run the internal quantum efficiency test. More... | |
| double | IQE_time_cutoff |
| Defines the simulation time cutoff for the internal quantum efficiency test. More... | |
| bool | Enable_dynamics_test |
| Specifies whether or not to run the dynamics test. More... | |
| bool | Enable_dynamics_extraction |
| Specifies whether or not to allow polaron extraction at the electrodes during the dynamics test. More... | |
| double | Dynamics_initial_exciton_conc |
| Defines the initial exciton concentration used by the dynamics test. More... | |
| double | Dynamics_transient_start |
| Defines the start time of the transient data collected during the dynamics test. More... | |
| double | Dynamics_transient_end |
| Defines the end time of the transient data collected during the dynamics test. More... | |
| int | Dynamics_pnts_per_decade |
| Defines the collected transient data time resolution in number of points per decade for the dynamics test. More... | |
| bool | Enable_steady_transport_test |
| Specifies whether or not the run the steady state charge transport test. More... | |
| double | Steady_carrier_density |
| Defines the steady state charge carrier density used by the steady state charge transport test. More... | |
| int | N_equilibration_events |
| Defines the number of events to execute during the equilibration phase of the steady charge transport test. More... | |
| bool | Enable_state_data_output = true |
| double | Exciton_generation_rate_donor |
| Defines the exciton generation rate on the donor sites is units of cm^-3 s^-3. More... | |
| double | Exciton_generation_rate_acceptor |
| Defines the exciton generation rate on the acceptor sites is units of cm^-3 s^-3. More... | |
| double | Singlet_lifetime_donor |
| Defines the singlet exciton lifetime when on the donor sites in units of seconds. More... | |
| double | Singlet_lifetime_acceptor |
| Defines the singlet exciton lifetime when on the acceptor sites in units of seconds. More... | |
| double | Triplet_lifetime_donor |
| Defines the triplet exciton lifetime when on the donor sites in units of seconds. More... | |
| double | Triplet_lifetime_acceptor |
| Defines the singlet exciton lifetime when on the acceptor sites in units of seconds. More... | |
| double | R_singlet_hopping_donor |
| Defines the singlet exciton hopping rate prefactor when on the donor sites in units of s^-1. More... | |
| double | R_singlet_hopping_acceptor |
| Defines the singlet exciton hopping rate prefactor when on the acceptor sites in units of s^-1. More... | |
| double | Singlet_localization_donor |
| Defines the singlet exciton localization parameter when on the donor sites in units of nm^-1. More... | |
| double | Singlet_localization_acceptor |
| Defines the singlet exciton localization parameter when on the acceptor sites in units of nm^-1. More... | |
| double | R_triplet_hopping_donor |
| Defines the triplet exciton hopping rate prefactor when on the donor sites in units of s^-1. More... | |
| double | R_triplet_hopping_acceptor |
| Defines the triplet exciton hopping rate prefactor when on the acceptor sites in units of s^-1. More... | |
| double | Triplet_localization_donor |
| Defines the triplet exciton localization parameter when on the donor sites in units of nm^-1. More... | |
| double | Triplet_localization_acceptor |
| Defines the triplet exciton localization parameter when on the acceptor sites in units of nm^-1. More... | |
| bool | Enable_FRET_triplet_annihilation |
| Specifies whether or not to use the FRET model for triplet annihilation events. More... | |
| double | R_exciton_exciton_annihilation_donor |
| Defines the exciton-exciton annihilation rate prefactor when starting from a donor site in units of s^-1. More... | |
| double | R_exciton_exciton_annihilation_acceptor |
| Defines the exciton-exciton annihilation rate prefactor when starting from an acceptor site in units of s^-1. More... | |
| double | R_exciton_polaron_annihilation_donor |
| Defines the exciton-polaron annihilation rate prefactor when starting from a donor site in units of s^-1. More... | |
| double | R_exciton_polaron_annihilation_acceptor |
| Defines the exciton-polaron annihilation rate prefactor when starting from an acceptor site in units of s^-1. More... | |
| int | FRET_cutoff |
| Defines the cutoff radius for FRET-based exciton mechanisms in units of nm. More... | |
| double | E_exciton_binding_donor |
| Defines the binding energy of excitons on donor sites in units of eV. More... | |
| double | E_exciton_binding_acceptor |
| Defines the binding energy of excitons on acceptor sites in units of eV. More... | |
| double | R_exciton_dissociation_donor |
| Defines the exciton dissociation rate prefactor for excitons starting on a donor site in units of s^-1. More... | |
| double | R_exciton_dissociation_acceptor |
| Defines the exciton dissociation rate prefactor for excitons starting on an acceptor site in units of s^-1. More... | |
| int | Exciton_dissociation_cutoff |
| Defines the cutoff radius for exciton dissociation events in units of nm. More... | |
| double | R_exciton_isc_donor |
| Defines the intersystem crossing (singlet to triplet) rate constant of excitons on donor sites in units of s^-1. More... | |
| double | R_exciton_isc_acceptor |
| Defines the intersystem crossing (singlet to triplet) rate constant of excitons on acceptor sites in units of s^-1. More... | |
| double | R_exciton_risc_donor |
| Defines the reverse intersystem crossing (triplet to singlet) rate constant of excitons on donor sites in units of s^-1. More... | |
| double | R_exciton_risc_acceptor |
| Defines the reverse intersystem crossing (triplet to singlet) rate constant of excitons on acceptor sites in units of s^-1. More... | |
| double | E_exciton_ST_donor |
| Defines the potential energy difference between singlet and triplet exciton states on donor sites in units of eV. More... | |
| double | E_exciton_ST_acceptor |
| Defines the potential energy difference between singlet and triplet exciton states on acceptor sites in units of eV. More... | |
| bool | Enable_phase_restriction |
| Specifies whether or not holes will be restricted to donor sites and electrons to acceptor sites. More... | |
| double | R_polaron_hopping_donor |
| Defines the polaron hopping rate prefactor of polarons on donor sites in units of s^-1. More... | |
| double | R_polaron_hopping_acceptor |
| Defines the polaron hopping rate prefactor of polarons on acceptor sites in units of s^-1. More... | |
| double | Polaron_localization_donor |
| Defines the polaron localization parameter when on the donor sites in units of nm^-1. More... | |
| double | Polaron_localization_acceptor |
| Defines the polaron localization parameter when on the acceptor sites in units of nm^-1. More... | |
| bool | Enable_miller_abrahams |
| Specifies whether or not to use the Miller-Abrahams model for polaron hopping events. More... | |
| bool | Enable_marcus |
| Specifies whether or not the use the Marcus model for polaron hopping events. More... | |
| double | Reorganization_donor |
| Defines the reorganization energy parameter used by the Marcus model for polaron hopping rates when on the donor sites in units of eV. More... | |
| double | Reorganization_acceptor |
| Defines the reorganization energy parameter used by the Marcus model for polaron hopping rates when on the acceptor sites in units of eV. More... | |
| double | R_polaron_recombination |
| Defines the polaron recombination rate prefactor in units of s^-1. More... | |
| int | Polaron_hopping_cutoff |
| Defines the cutoff radius of all polaron hopping events in units of nm. More... | |
| bool | Enable_gaussian_polaron_delocalization |
| Specifies whether or not to use the Gaussian polaron delocalization model. More... | |
| double | Polaron_delocalization_length |
| Defines the polaron delocalization length used by the Gaussian polaron delocalization model. More... | |
| double | Homo_donor |
| Defines the highest occupied molecular orbital energy of the donor sites in units of eV. More... | |
| double | Lumo_donor |
| Defines the lowest unoccupied molecular orbital energy of the donor sites in units of eV. More... | |
| double | Homo_acceptor |
| Defines the highest occupied molecular orbital energy of the acceptor sites in units of eV. More... | |
| double | Lumo_acceptor |
| Defines the lowest unoccupied molecular orbital energy of the acceptor sites in units of eV. More... | |
| bool | Enable_gaussian_dos |
| Specifies whether or not to use the Gaussian density of states model to define the site energies. More... | |
| double | Energy_stdev_donor |
| Defines the standard deviation of the donor site energy distribution used by the Gaussian density of states model in units of eV. More... | |
| double | Energy_stdev_acceptor |
| Defines the standard deviation of the acceptor site energy distribution used by the Gaussian density of states model in units of eV. More... | |
| bool | Enable_exponential_dos |
| Specifies whether or not to use the exponential density of states model to define the site energies. More... | |
| double | Energy_urbach_donor |
| Defines the Urbach energy of the donor site energy distribution used by the exponential density of states model in units of eV. More... | |
| double | Energy_urbach_acceptor |
| Defines the Urbach energy of the acceptor site energy distribution used by the exponential density of states model in units of eV. More... | |
| bool | Enable_correlated_disorder |
| Specifies whether or not the use the correlated Gaussian disorder model to define the site energies. More... | |
| double | Disorder_correlation_length |
| Defines the desired correlation length for the correlated Gaussian disorder model in units of nm. More... | |
| bool | Enable_gaussian_kernel |
| Specifies whether or not to use the Gaussian kernel with the correlated Gaussian density of states model. More... | |
| bool | Enable_power_kernel |
| Specifies whether or not to use the power kernel with the correlated Gaussian density of states model. More... | |
| int | Power_kernel_exponent |
| Defines the power kernel exponent to be used with the power kernel correlated Gaussian density of states model. More... | |
| bool | Enable_interfacial_energy_shift |
| Specifies whether or not to use the interfacial energy shift model to modify the site energies. More... | |
| double | Energy_shift_donor |
| Defines the energy shift parameter for the donor sites used by the interfacial energy shift model in units of eV. More... | |
| double | Energy_shift_acceptor |
| Defines the energy shift parameter for the acceptor sites used by the interfacial energy shift model in units of eV. More... | |
| bool | Enable_import_energies |
| Specifies whether or not to import the site energies from a text file. More... | |
| std::string | Energies_import_filename |
| The name of site energy text file to be imported. More... | |
| double | Dielectric_donor |
| Defines the dielectric constant of the donor sites. More... | |
| double | Dielectric_acceptor |
| Defines the dielectric constant of the acceptor sites. More... | |
| int | Coulomb_cutoff |
| Defines the cutoff radius for Coulomb interactions in units of nm. More... | |
| Public Attributes inherited from KMC_Lattice::Parameters_Simulation | |
| Parameters_Lattice | Params_lattice |
| bool | Enable_logging = false |
| Determines whether logging to a logfile during the simulation will be enabled or not. More... | |
| int | Temperature = 0 |
| Defines the desired temperature of the simulation in Kelvin. More... | |
| bool | Enable_FRM = false |
| Determines whether the first reaction method will be used or not. More... | |
| bool | Enable_selective_recalc = false |
| Determines whether the selective recalculation method will be used or not. More... | |
| int | Recalc_cutoff = 0 |
| Defines the desired event recalculation cutoff radius for the simulation in nm. More... | |
| bool | Enable_full_recalc = false |
| Determines whether the full recalculation method will be used or not. More... | |
| std::ofstream * | Logfile = nullptr |
| Defines the desired output file stream pointer to the logfile. More... | |
This class extends the KMC_Lattice::Parameters_Simulation class to create a parameters object that holds all input parameters needed by a simulation.
| bool Excimontec::Parameters::checkParameters | ( | ) | const |
Checks the validity of the current parameter values.
| bool Excimontec::Parameters::importParameters | ( | std::ifstream & | inputfile | ) |
Imports the values for all parameters by parsing the input filestream.
| inputfile | is an opened input filestream pointing to a valid parameter text file. |
| double Excimontec::Parameters::Acceptor_conc |
Defines the acceptor site volume concentration when using the random blend device architecture.
| int Excimontec::Parameters::Coulomb_cutoff |
Defines the cutoff radius for Coulomb interactions in units of nm.
| double Excimontec::Parameters::Dielectric_acceptor |
Defines the dielectric constant of the acceptor sites.
| double Excimontec::Parameters::Dielectric_donor |
Defines the dielectric constant of the donor sites.
| double Excimontec::Parameters::Disorder_correlation_length |
Defines the desired correlation length for the correlated Gaussian disorder model in units of nm.
| double Excimontec::Parameters::Dynamics_initial_exciton_conc |
Defines the initial exciton concentration used by the dynamics test.
| int Excimontec::Parameters::Dynamics_pnts_per_decade |
Defines the collected transient data time resolution in number of points per decade for the dynamics test.
| double Excimontec::Parameters::Dynamics_transient_end |
Defines the end time of the transient data collected during the dynamics test.
| double Excimontec::Parameters::Dynamics_transient_start |
Defines the start time of the transient data collected during the dynamics test.
| double Excimontec::Parameters::E_exciton_binding_acceptor |
Defines the binding energy of excitons on acceptor sites in units of eV.
| double Excimontec::Parameters::E_exciton_binding_donor |
Defines the binding energy of excitons on donor sites in units of eV.
| double Excimontec::Parameters::E_exciton_ST_acceptor |
Defines the potential energy difference between singlet and triplet exciton states on acceptor sites in units of eV.
| double Excimontec::Parameters::E_exciton_ST_donor |
Defines the potential energy difference between singlet and triplet exciton states on donor sites in units of eV.
| bool Excimontec::Parameters::Enable_bilayer |
Specifies whether or not to use a bilayer device architecture.
| bool Excimontec::Parameters::Enable_correlated_disorder |
Specifies whether or not the use the correlated Gaussian disorder model to define the site energies.
| bool Excimontec::Parameters::Enable_dynamics_extraction |
Specifies whether or not to allow polaron extraction at the electrodes during the dynamics test.
| bool Excimontec::Parameters::Enable_dynamics_test |
Specifies whether or not to run the dynamics test.
| bool Excimontec::Parameters::Enable_exciton_diffusion_test |
Specifies whether or not the exciton diffusion test is to be run.
| bool Excimontec::Parameters::Enable_exponential_dos |
Specifies whether or not to use the exponential density of states model to define the site energies.
| bool Excimontec::Parameters::Enable_extraction_map_output = false |
Specifies whether or not extraction map data should be output to text file at the end of the simulation.
| bool Excimontec::Parameters::Enable_FRET_triplet_annihilation |
Specifies whether or not to use the FRET model for triplet annihilation events.
| bool Excimontec::Parameters::Enable_gaussian_dos |
Specifies whether or not to use the Gaussian density of states model to define the site energies.
| bool Excimontec::Parameters::Enable_gaussian_kernel |
Specifies whether or not to use the Gaussian kernel with the correlated Gaussian density of states model.
| bool Excimontec::Parameters::Enable_gaussian_polaron_delocalization |
Specifies whether or not to use the Gaussian polaron delocalization model.
| bool Excimontec::Parameters::Enable_import_energies |
Specifies whether or not to import the site energies from a text file.
| bool Excimontec::Parameters::Enable_import_morphology |
Specifies whether or not an imported morphology is being used to define the device architecture.
| bool Excimontec::Parameters::Enable_import_morphology_set = false |
Specifies whether or not to import a set of morphologies to be assigned to different processors.
| bool Excimontec::Parameters::Enable_import_morphology_single = false |
Specifies whether or not to import a single morphology file and use it on all processors.
| bool Excimontec::Parameters::Enable_interfacial_energy_shift |
Specifies whether or not to use the interfacial energy shift model to modify the site energies.
| bool Excimontec::Parameters::Enable_IQE_test |
Specifies whether or not to run the internal quantum efficiency test.
| bool Excimontec::Parameters::Enable_marcus |
Specifies whether or not the use the Marcus model for polaron hopping events.
| bool Excimontec::Parameters::Enable_miller_abrahams |
Specifies whether or not to use the Miller-Abrahams model for polaron hopping events.
| bool Excimontec::Parameters::Enable_neat |
Specifies whether or not to use a neat single phase material device architecture. A neat material morphology uses the donor material properties.
| bool Excimontec::Parameters::Enable_phase_restriction |
Specifies whether or not holes will be restricted to donor sites and electrons to acceptor sites.
| bool Excimontec::Parameters::Enable_power_kernel |
Specifies whether or not to use the power kernel with the correlated Gaussian density of states model.
| bool Excimontec::Parameters::Enable_random_blend |
Specifies whether or not to use a random blend material device architecture.
| bool Excimontec::Parameters::Enable_state_data_output = true |
Specifies whether or not to output the density of occupied states and density of states data after the steady state charge transport test.
| bool Excimontec::Parameters::Enable_steady_transport_test |
Specifies whether or not the run the steady state charge transport test.
| bool Excimontec::Parameters::Enable_ToF_energy_placement |
Specifies whether or not to use the energy placement method for creating the initial polarons in the time-of-flight charge transport test.
| bool Excimontec::Parameters::Enable_ToF_random_placement |
Specifies whether or not to use the random placement method for creating the initial polarons in the time-of-flight charge transport test.
| bool Excimontec::Parameters::Enable_ToF_test |
Specifies whether or not to run the time-of-flight charge transport test.
| std::string Excimontec::Parameters::Energies_import_filename |
The name of site energy text file to be imported.
| double Excimontec::Parameters::Energy_shift_acceptor |
Defines the energy shift parameter for the acceptor sites used by the interfacial energy shift model in units of eV.
| double Excimontec::Parameters::Energy_shift_donor |
Defines the energy shift parameter for the donor sites used by the interfacial energy shift model in units of eV.
| double Excimontec::Parameters::Energy_stdev_acceptor |
Defines the standard deviation of the acceptor site energy distribution used by the Gaussian density of states model in units of eV.
| double Excimontec::Parameters::Energy_stdev_donor |
Defines the standard deviation of the donor site energy distribution used by the Gaussian density of states model in units of eV.
| double Excimontec::Parameters::Energy_urbach_acceptor |
Defines the Urbach energy of the acceptor site energy distribution used by the exponential density of states model in units of eV.
| double Excimontec::Parameters::Energy_urbach_donor |
Defines the Urbach energy of the donor site energy distribution used by the exponential density of states model in units of eV.
| int Excimontec::Parameters::Exciton_dissociation_cutoff |
Defines the cutoff radius for exciton dissociation events in units of nm.
| double Excimontec::Parameters::Exciton_generation_rate_acceptor |
Defines the exciton generation rate on the acceptor sites is units of cm^-3 s^-3.
| double Excimontec::Parameters::Exciton_generation_rate_donor |
Defines the exciton generation rate on the donor sites is units of cm^-3 s^-3.
| int Excimontec::Parameters::FRET_cutoff |
Defines the cutoff radius for FRET-based exciton mechanisms in units of nm.
| double Excimontec::Parameters::Homo_acceptor |
Defines the highest occupied molecular orbital energy of the acceptor sites in units of eV.
| double Excimontec::Parameters::Homo_donor |
Defines the highest occupied molecular orbital energy of the donor sites in units of eV.
| double Excimontec::Parameters::Internal_potential |
Defines the internal electrical potential across the semiconductor layer.
| double Excimontec::Parameters::IQE_time_cutoff |
Defines the simulation time cutoff for the internal quantum efficiency test.
| double Excimontec::Parameters::Lumo_acceptor |
Defines the lowest unoccupied molecular orbital energy of the acceptor sites in units of eV.
| double Excimontec::Parameters::Lumo_donor |
Defines the lowest unoccupied molecular orbital energy of the donor sites in units of eV.
| std::string Excimontec::Parameters::Morphology_filename |
The name of the morphology file to be imported.
| std::string Excimontec::Parameters::Morphology_set_format = "" |
Defines the morphology set naming format. The standard naming format is morphology_#.txt where # is a wildcard for different numbers.
| int Excimontec::Parameters::N_equilibration_events |
Defines the number of events to execute during the equilibration phase of the steady charge transport test.
| int Excimontec::Parameters::N_morphology_set_size = 0 |
Defines the number of morphologies in the set. It is assumed that morphologies in the set are number from 0 to N_morphology_set_size-1.
| int Excimontec::Parameters::N_test_morphologies = 0 |
Defines the number of morphologies to be tested from the set.
| int Excimontec::Parameters::N_tests |
Used as a generic counter for determining when a given simulation test is completed.
| double Excimontec::Parameters::Polaron_delocalization_length |
Defines the polaron delocalization length used by the Gaussian polaron delocalization model.
| int Excimontec::Parameters::Polaron_hopping_cutoff |
Defines the cutoff radius of all polaron hopping events in units of nm.
| double Excimontec::Parameters::Polaron_localization_acceptor |
Defines the polaron localization parameter when on the acceptor sites in units of nm^-1.
| double Excimontec::Parameters::Polaron_localization_donor |
Defines the polaron localization parameter when on the donor sites in units of nm^-1.
| int Excimontec::Parameters::Power_kernel_exponent |
Defines the power kernel exponent to be used with the power kernel correlated Gaussian density of states model.
| double Excimontec::Parameters::R_exciton_dissociation_acceptor |
Defines the exciton dissociation rate prefactor for excitons starting on an acceptor site in units of s^-1.
| double Excimontec::Parameters::R_exciton_dissociation_donor |
Defines the exciton dissociation rate prefactor for excitons starting on a donor site in units of s^-1.
| double Excimontec::Parameters::R_exciton_exciton_annihilation_acceptor |
Defines the exciton-exciton annihilation rate prefactor when starting from an acceptor site in units of s^-1.
| double Excimontec::Parameters::R_exciton_exciton_annihilation_donor |
Defines the exciton-exciton annihilation rate prefactor when starting from a donor site in units of s^-1.
| double Excimontec::Parameters::R_exciton_isc_acceptor |
Defines the intersystem crossing (singlet to triplet) rate constant of excitons on acceptor sites in units of s^-1.
| double Excimontec::Parameters::R_exciton_isc_donor |
Defines the intersystem crossing (singlet to triplet) rate constant of excitons on donor sites in units of s^-1.
| double Excimontec::Parameters::R_exciton_polaron_annihilation_acceptor |
Defines the exciton-polaron annihilation rate prefactor when starting from an acceptor site in units of s^-1.
| double Excimontec::Parameters::R_exciton_polaron_annihilation_donor |
Defines the exciton-polaron annihilation rate prefactor when starting from a donor site in units of s^-1.
| double Excimontec::Parameters::R_exciton_risc_acceptor |
Defines the reverse intersystem crossing (triplet to singlet) rate constant of excitons on acceptor sites in units of s^-1.
| double Excimontec::Parameters::R_exciton_risc_donor |
Defines the reverse intersystem crossing (triplet to singlet) rate constant of excitons on donor sites in units of s^-1.
| double Excimontec::Parameters::R_polaron_hopping_acceptor |
Defines the polaron hopping rate prefactor of polarons on acceptor sites in units of s^-1.
| double Excimontec::Parameters::R_polaron_hopping_donor |
Defines the polaron hopping rate prefactor of polarons on donor sites in units of s^-1.
| double Excimontec::Parameters::R_polaron_recombination |
Defines the polaron recombination rate prefactor in units of s^-1.
| double Excimontec::Parameters::R_singlet_hopping_acceptor |
Defines the singlet exciton hopping rate prefactor when on the acceptor sites in units of s^-1.
| double Excimontec::Parameters::R_singlet_hopping_donor |
Defines the singlet exciton hopping rate prefactor when on the donor sites in units of s^-1.
| double Excimontec::Parameters::R_triplet_hopping_acceptor |
Defines the triplet exciton hopping rate prefactor when on the acceptor sites in units of s^-1.
| double Excimontec::Parameters::R_triplet_hopping_donor |
Defines the triplet exciton hopping rate prefactor when on the donor sites in units of s^-1.
| double Excimontec::Parameters::Reorganization_acceptor |
Defines the reorganization energy parameter used by the Marcus model for polaron hopping rates when on the acceptor sites in units of eV.
| double Excimontec::Parameters::Reorganization_donor |
Defines the reorganization energy parameter used by the Marcus model for polaron hopping rates when on the donor sites in units of eV.
| double Excimontec::Parameters::Singlet_lifetime_acceptor |
Defines the singlet exciton lifetime when on the acceptor sites in units of seconds.
| double Excimontec::Parameters::Singlet_lifetime_donor |
Defines the singlet exciton lifetime when on the donor sites in units of seconds.
| double Excimontec::Parameters::Singlet_localization_acceptor |
Defines the singlet exciton localization parameter when on the acceptor sites in units of nm^-1.
| double Excimontec::Parameters::Singlet_localization_donor |
Defines the singlet exciton localization parameter when on the donor sites in units of nm^-1.
| double Excimontec::Parameters::Steady_carrier_density |
Defines the steady state charge carrier density used by the steady state charge transport test.
| int Excimontec::Parameters::Thickness_acceptor |
Defines the acceptor layer thickness in number of sites when using bilayer architecture.
| int Excimontec::Parameters::Thickness_donor |
Defines the donor layer thickness in number of sites when using bilayer architecture.
| int Excimontec::Parameters::ToF_initial_polarons |
Defines the number of initial polarons to place in the simulation for the time-of-flight charge transport test.
| double Excimontec::Parameters::ToF_placement_energy |
Defines the preferred energy within the DOS for initial polaron placement when using the energy placement method with the time-of-flight charge transport test.
| int Excimontec::Parameters::ToF_pnts_per_decade |
Defines the collected transient data time resolution in number of points per decade for the time-of-flight charge transport test.
| bool Excimontec::Parameters::ToF_polaron_type |
Specifies the type of polaron to test when performing the time-of-flight charge transport test. (false for electron and true for hole)
| double Excimontec::Parameters::ToF_transient_end |
Defines the end time of the transient data collected during the time-of-flight charge transport test.
| double Excimontec::Parameters::ToF_transient_start |
Defines the start time of the transient data collected during the time-of-flight charge transport test.
| double Excimontec::Parameters::Triplet_lifetime_acceptor |
Defines the singlet exciton lifetime when on the acceptor sites in units of seconds.
| double Excimontec::Parameters::Triplet_lifetime_donor |
Defines the triplet exciton lifetime when on the donor sites in units of seconds.
| double Excimontec::Parameters::Triplet_localization_acceptor |
Defines the triplet exciton localization parameter when on the acceptor sites in units of nm^-1.
| double Excimontec::Parameters::Triplet_localization_donor |
Defines the triplet exciton localization parameter when on the donor sites in units of nm^-1.


Markdown Headers
Over the past few weeks, I’ve been writing a lot more in Markdown. Markdown is simple and easy to use, as I’ve pointed out before.
Whilst nValt offers a good search function to find data within a note, I’ve been exploring additional details that I could add to files to make them easier to find. Well, it turns out that MultiMarkdown supports meta data or headers, something I didn’t realise even though I use MMD more than vanilla Markdown more often than not!
Anyhow, creating the headers can be a bit repetitive, so I looked into how I could change that. Obviously, this relies on the fantastic Keyboard Maestro on my Mac but the iPad version relies on Editorial, as that’s where I tend to do the majority of my work.
The headers are stripped from the final document if viewed in either nValt’s preview window or Marked so they don’t appear. However, it makes it a bit easier to search.
Keyboard Maestro
The Keyboard Maestro macro was the easiest option to create - running it provides a text prompt for the user to input the title and to select the document type. This is then pasted into the document.
Editorial
I created an Editorial workflow to create the headers (viewable here). It’s the same as the Keyboard Maestro version, however, I teamed this up with Launch Centre Pro.
When I want to create a post in Editorial, I now load up Launch Centre Pro and select the option with the following URL.
<code>editorial://new/{{[prompt:Filename].md}}?root={{Dropbox}}&command={{Markdown Header}}
</code>
This runs the linked workflow and fills in the basic Markdown headers.
This should therefore help me to create documents and allow me to search them a bit easier. I’ll see how it pans out over the next few weeks. The issue above is Windows, which seems to be the short link in most things. Maybe I should start learning AutoHotKey syntax more as that might be able to do what I want.


South Florida man claims wind blew cocaine into his car, police say
by Bob D'Angelo, Cox Media Group National Content DeskThe answer, a South Florida man told police, was blowing in the wind.
Joseph Jeffery Zak, 37, of Port St. Lucie, is facing a misdemeanor drug charge after he told police wind blew a bag of cocaine into his car, WPEC reported.
According to an arrest affidavit filed by the Fort Pierce Police Department, Zak was pulled over by authorities at 11:40 p.m. Oct. 30 when he failed to stop at an intersection.
Police said Zak made movements in an attempt to throw something away from the vehicle's center console, the affidavit said.
According to the arrest affidavit, a search of the sedan Zak was driving revealed a crack pipe in the center console and a clear baggie filled with a white substance, WPEC reported. Police said the substance tested positive for crack cocaine, according to the arrest affidavit.
According to police, Zak said the baggie did not belong to him, asserting the "police or the wind must have placed it there," the affidavit said.
Police charged Zak with possession of paraphernalia Oct. 31, and he was taken to the St. Lucie County Jail, WPEC reported. He is expected in court Dec. 3.


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