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

Binary file not shown.

After

Width:  |  Height:  |  Size: 9.2 KiB

Binary file not shown.

After

Width:  |  Height:  |  Size: 9.1 KiB

Binary file not shown.

Before

Width:  |  Height:  |  Size: 8.1 KiB

After

Width:  |  Height:  |  Size: 9.4 KiB

Binary file not shown.

Before

Width:  |  Height:  |  Size: 8.5 KiB

After

Width:  |  Height:  |  Size: 10 KiB

Binary file not shown.

Before

Width:  |  Height:  |  Size: 7.5 KiB

After

Width:  |  Height:  |  Size: 9.2 KiB

Binary file not shown.

Before

Width:  |  Height:  |  Size: 7.1 KiB

After

Width:  |  Height:  |  Size: 8.8 KiB

Binary file not shown.

Before

Width:  |  Height:  |  Size: 8.0 KiB

After

Width:  |  Height:  |  Size: 9.4 KiB

Binary file not shown.

Before

Width:  |  Height:  |  Size: 8.0 KiB

After

Width:  |  Height:  |  Size: 9.5 KiB

Binary file not shown.

Before

Width:  |  Height:  |  Size: 8.0 KiB

After

Width:  |  Height:  |  Size: 9.5 KiB

View File

@ -25,28 +25,36 @@ Schrödinger's equation: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^
---
jkqtmathtext_fira.png
--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
--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
--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
--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
--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
--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
--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: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$

View File

@ -181,6 +181,8 @@ class JKQTMathTextNode; // forward
<br>using "Computer Modern": \image html jkqtmathtext/jkqtmathtext_computermodern.png
<br>using "Fira": \image html jkqtmathtext/jkqtmathtext_fira.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: