diff --git a/doc/images/jkqtmathtext/jkqtmathtext_DejaVuSans.png b/doc/images/jkqtmathtext/jkqtmathtext_DejaVuSans.png new file mode 100644 index 0000000000..a74ab3f2c6 Binary files /dev/null and b/doc/images/jkqtmathtext/jkqtmathtext_DejaVuSans.png differ diff --git a/doc/images/jkqtmathtext/jkqtmathtext_DejaVuSerif.png b/doc/images/jkqtmathtext/jkqtmathtext_DejaVuSerif.png new file mode 100644 index 0000000000..4c9811ec48 Binary files /dev/null and b/doc/images/jkqtmathtext/jkqtmathtext_DejaVuSerif.png differ diff --git a/doc/images/jkqtmathtext/jkqtmathtext_asana.png b/doc/images/jkqtmathtext/jkqtmathtext_asana.png index 92e47d260d..4a19ef83e2 100644 Binary files a/doc/images/jkqtmathtext/jkqtmathtext_asana.png and b/doc/images/jkqtmathtext/jkqtmathtext_asana.png differ diff --git a/doc/images/jkqtmathtext/jkqtmathtext_computermodern.png b/doc/images/jkqtmathtext/jkqtmathtext_computermodern.png index fc6878c55d..e941f3fde9 100644 Binary files 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b/doc/images/jkqtmathtext/jkqtmathtext_xits.png index a196a996b3..17cd51afaa 100644 Binary files a/doc/images/jkqtmathtext/jkqtmathtext_xits.png and b/doc/images/jkqtmathtext/jkqtmathtext_xits.png differ diff --git a/doc/images/jkqtmathtext/jkqtmathtext_xits_all.png b/doc/images/jkqtmathtext/jkqtmathtext_xits_all.png index a196a996b3..17cd51afaa 100644 Binary files a/doc/images/jkqtmathtext/jkqtmathtext_xits_all.png and b/doc/images/jkqtmathtext/jkqtmathtext_xits_all.png differ diff --git a/doc/jkqtmathtext_docimages_specialfonts.jkmt b/doc/jkqtmathtext_docimages_specialfonts.jkmt index 7f0dcaf761..6e027e250b 100644 --- a/doc/jkqtmathtext_docimages_specialfonts.jkmt +++ b/doc/jkqtmathtext_docimages_specialfonts.jkmt @@ -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: $\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2}+V\right]\Psi(x)=\mathrm{i}\hbar\frac{\partial}{\partial t}\Psi(x),\ \ x\in\mathbb{R}, \Psi(x)\in\mathbb{C}$ diff --git a/lib/jkqtmathtext/jkqtmathtext.h b/lib/jkqtmathtext/jkqtmathtext.h index 7aed476aca..519488c6a1 100644 --- a/lib/jkqtmathtext/jkqtmathtext.h +++ b/lib/jkqtmathtext/jkqtmathtext.h @@ -181,6 +181,8 @@ class JKQTMathTextNode; // forward
using "Computer Modern": \image html jkqtmathtext/jkqtmathtext_computermodern.png
using "Fira": \image html jkqtmathtext/jkqtmathtext_fira.png
using "MS Segoe UI": \image html jkqtmathtext/jkqtmathtext_mssegoeui.png +
using "DejaVu Sans": \image html jkqtmathtext/jkqtmathtext_DejaVuSans.png +
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: