doc-update

This commit is contained in:
jkriege2 2022-08-10 14:41:26 +02:00
parent c917b53886
commit 9ab3ddd3b0
11 changed files with 17 additions and 7 deletions

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@ -25,28 +25,36 @@ Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^
--- ---
jkqtmathtext_fira.png jkqtmathtext_fira.png
--fontmathroman=Fira Math --fontroman=Fira Sans --sizeincrease=10 --fontmathroman=Fira Math --fontroman=Fira Sans --sizeincrease=10
Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x)$ Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$
---
jkqtmathtext_DejaVuSerif.png
--fontmathroman=DejaVu Serif --fontroman=DejaVu Serif --fontfallbacksymbol=DejaVu Serif --sizeincrease=10
Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$
---
jkqtmathtext_DejaVuSans.png
--fontmathroman=DejaVu Sans --fontroman=DejaVu Sans --fontfallbacksymbol=DejaVu Sans --sizeincrease=10
Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$
--- ---
jkqtmathtext_mssegoeui.png jkqtmathtext_mssegoeui.png
--fontmathroman=Segoe UI --fontroman=Segoe UI --fontfallbacksymbol=Segoe UI Symbol --sizeincrease=10 --fontmathroman=Segoe UI --fontroman=Segoe UI --fontfallbacksymbol=Segoe UI Symbol --sizeincrease=10
Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x)$ Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$
--- ---
jkqtmathtext_computermodern.png jkqtmathtext_computermodern.png
--fontmathroman=CMU Serif --fontroman=SMU Serif --sizeincrease=10 --fontmathroman=CMU Serif --fontroman=SMU Serif --sizeincrease=10
Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x)$ Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$
--- ---
jkqtmathtext_asana.png jkqtmathtext_asana.png
--fontmathroman=Asana Math --sizeincrease=10 --fontmathroman=Asana Math --sizeincrease=10
Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x)$ Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$
--- ---
jkqtmathtext_xits_all.png jkqtmathtext_xits_all.png
--fontroman=XITS --fontmathroman=XITS Math --sizeincrease=10 --fontroman=XITS --fontmathroman=XITS Math --sizeincrease=10
Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x)$ Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$
--- ---
jkqtmathtext_xits.png jkqtmathtext_xits.png
--fontmathroman=XITS Math --sizeincrease=10 --fontmathroman=XITS Math --sizeincrease=10
Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x)$ Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$
--- ---
jkqtmathtext_stix.png jkqtmathtext_stix.png
--fontmathroman=STIX Two Math --fontroman=STIX Two Text --sizeincrease=10 --fontmathroman=STIX Two Math --fontroman=STIX Two Text --sizeincrease=10
Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x)$ Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$

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@ -181,6 +181,8 @@ class JKQTMathTextNode; // forward
<br>using "Computer Modern": \image html jkqtmathtext/jkqtmathtext_computermodern.png <br>using "Computer Modern": \image html jkqtmathtext/jkqtmathtext_computermodern.png
<br>using "Fira": \image html jkqtmathtext/jkqtmathtext_fira.png <br>using "Fira": \image html jkqtmathtext/jkqtmathtext_fira.png
<br>using "MS Segoe UI": \image html jkqtmathtext/jkqtmathtext_mssegoeui.png <br>using "MS Segoe UI": \image html jkqtmathtext/jkqtmathtext_mssegoeui.png
<br>using "DejaVu Sans": \image html jkqtmathtext/jkqtmathtext_DejaVuSans.png
<br>using "DejaVu Serif": \image html jkqtmathtext/jkqtmathtext_DejaVuSerif.png
. .
Math-mode is activated by enclosing your equation in \c $...$ or \c \\[...\\] . This mode is optimized for mathematical equations. Here is an example of the difference: Math-mode is activated by enclosing your equation in \c $...$ or \c \\[...\\] . This mode is optimized for mathematical equations. Here is an example of the difference: