doc-update
BIN
doc/images/jkqtmathtext/jkqtmathtext_DejaVuSans.png
Normal file
After Width: | Height: | Size: 9.2 KiB |
BIN
doc/images/jkqtmathtext/jkqtmathtext_DejaVuSerif.png
Normal file
After Width: | Height: | Size: 9.1 KiB |
Before Width: | Height: | Size: 8.1 KiB After Width: | Height: | Size: 9.4 KiB |
Before Width: | Height: | Size: 8.5 KiB After Width: | Height: | Size: 10 KiB |
Before Width: | Height: | Size: 7.5 KiB After Width: | Height: | Size: 9.2 KiB |
Before Width: | Height: | Size: 7.1 KiB After Width: | Height: | Size: 8.8 KiB |
Before Width: | Height: | Size: 8.0 KiB After Width: | Height: | Size: 9.4 KiB |
Before Width: | Height: | Size: 8.0 KiB After Width: | Height: | Size: 9.5 KiB |
Before Width: | Height: | Size: 8.0 KiB After Width: | Height: | Size: 9.5 KiB |
@ -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: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$
|
||||
|
@ -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:
|
||||
|