image imagewidth (px) 24 1.05k | text stringlengths 2 982 | class stringclasses 2
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ααΆααΆααααααααΌαααααΎα’αααΈα | khmer | |
\rho^2 \ln(\Lambda l)^2 \ll \frac{1}{l^2} \ln\frac{1}{(\rho l)^2}\label{eq20} | expression | |
S^{\rm W}(p) = -i\gamma\cdot p \sigma_{V}^{\rm W}(p) \label{Csym} | expression | |
{}\label{hamac}S^G [h_{ij}, \pi^{ij}, N, N^i] = \int_{\cal M} dt \, d^3x \left( {\pi}^{ij} {\dot h}_{ij} - N H^G - N^i H^G_i \right), | expression | |
ααααβααΆαα· | khmer | |
X^{A{A^\prime}}_{0}:=i{\sqrt2}(\sigma^{A} \beta^{A^\prime}- \varsigma^{A} \alpha^{A^\prime})=-i{\sqrt2}({\bar \sigma}^{A^\prime}{\bar \beta}^{A} -{\bar \varsigma}^{A^\prime}{\bar \alpha}^{A}), | expression | |
P[R>s]\ \ge\ \lim_{m\to\infty} P[\cap_{n\ge m}A_n(t^{2n})^c]\ . | expression | |
\Gamma(b_1 \to \gamma + \gamma)= \zeta \left({M_1\over2m_P}\right)^4 \left({A\over\ell_P^2}\right)^2{M_1\over2\hbar}. | expression | |
αα·ααααΆααΆα | khmer | |
αααα | khmer | |
ααα»ααααΆα? | khmer | |
αααΎαα·αααα·ααΆαααααα·α
αα
αα·α | khmer | |
{\widehat \Gamma}_{\; \; \; BC}^{A'} \equiv \Gamma_{\; \; \; BC}^{A'}+\nabla_{\; \; \; B}^{A'} \; \nu_{C} \; , | expression | |
\lambda^2 - \mbox{Tr} Z \, \lambda +\mbox{det}Z =0 \label{simple} | expression | |
straight for the nearest | khmer | |
\label{5} [x_0, x_i] = -\frac{i}{\kappa}\, x_i, \quad [x_i, x_j] = 0., | expression | |
{\cal L} = - \frac{1}{4} F^a_{\mu\nu} F^{\mu\nu,a} + \frac{1}{2}m^2A_\mu^aA^{\mu,a} \label{4.1} | expression | |
\bar{Z}(j) = 1 + \bar{X}(j\bar{Z}(j)), \;\;\;\;\;\; \bar{Z}(j) = \sum_{w}j^{\bar{w}}<\phi^{w}> \label{ff} | expression | |
D_i=\sum_j (X_{ji}^\dagger X_{ji}-X_{ij}X_{ij}^\dagger )=\theta_i,\label{eq:D-flatness} | expression | |
αα
αα·ααα
ααα’αα»αααααααααααΆα | khmer | |
x(t)=x_{r}(t)={1\over t},\quad y(t)=y_{r}(t)=-{1\over{t^2}}, \quad z(t)=z_{r}(t)=-{1\over{t^2}}. \label{eq:functions} | expression | |
\int_0^{\Delta t(r_P)} dt = \int_{r_P}^c e^{-r} dr. | expression | |
ααΆααααα | khmer | |
α‘α©α§α¦ α αα·αα·ααΆα αα·αααααααα ααααα·αααααΆ αα·αααααΆα αα·α αα ααααα·ααααα·ααΆα αα
α’αΆαααΈ | khmer | |
N^{AB}=\bar{\epsilon}_1\Gamma^{ABC}D_C\epsilon_2+\textstyle{1\over 8}\bar{\epsilon_1}\Gamma^{C_1C_2}\epsilon_2F^{AB}_{\ \ C_1C_2}+\textstyle{1\over{96}}\bar{\epsilon}_1\Gamma^{ABC_1\cdots C_4}\epsilon_2F_{C_1\cdots C_4}.\label{11dsgnester} | expression | |
\overline{g}=\sqrt{g^{2}+g^{\prime 2}} = \frac{1}{2\sqrt{\omega}}\sqrt{\tilde{g}^{2}+\tilde{g}^{\prime 2}} \label{VII34} | expression | |
α
ααα αααα
αα·α | khmer | |
\{w,z\} = \{w,u\}~(\frac{du}{dz})^{2} + \{u,z\} | expression | |
αααααΆαα·ααΆαααΆα | khmer | |
αααα½α
ααααΆαα | khmer | |
K_{i}E_{\alpha}=q^{(\alpha,\alpha_{i})}E_{\alpha}K_{i},K_{i}F_{\alpha}=q^{-(\alpha,\alpha_{i})}F_{\alpha}K_{i}, | expression | |
\label{obh:matter}{\delta L\over \delta\Psi} = {\partial L\over \partial\Psi} -(-1)^{p}D{\partial L \over \partial D\Psi}=0. | expression | |
%F_{2,a} - F_{2,-a}, F_{2,b} - F_{2,-b}%\label{5.16}% | expression | |
{\cal P} : T \mapsto -T, \qquad Q_\pm \mapsto\bar{Q}_\mp , \qquad \bar{Q}_\pm \mapsto Q_\mp\,. | expression | |
F(g)= -\frac{3}{8} -\frac{5 A^2}{48}-\frac{A^4}{384} -\frac{1}{2} \log\frac{A^2}{4} + \frac{C_1}{g^2},\label{sol1} | expression | |
\Psi_D =\left( \begin{array}{c}A\\B\\C\\D\end{array} \right). | expression | |
\label{quater.constr.}\phi_2^4=\frac{\sqrt{g}}{\alpha}\left[p_1^2-m^2+\sqrt{g}~\frac{\alpha m+\beta\sigma\sqrt{m^2-p_1^2}}{(q_2^2)^{3/2}}\right],~~~~~~\sigma=\mbox{sign}~\varepsilon(p_1q_2q_3), | expression | |
αααααΆααΆα
αΆαα·ααααααΆααα’αααα | khmer | |
ααΆα αα½ααΆααΈ ααΆ αααααααα·ααΆααααα ααα | khmer | |
E_{eff(3+1)}=-\frac{1}{2\pi^{2}}\int_{0}^{+\infty}k\ln\left(\frac{k^{2}+m^{2}_{f}}{m_{f}^{2}}\right) (\Delta(k)-c) dk | expression | |
[\partial_A-\Phi_A,\partial_B-\Phi_B]=\partial_B\Phi_A-\partial_A\Phi_B+[\Phi_A,\Phi_B]=0 | expression | |
{\sum_{j=1}^{m+1} \sum_{k=0}^{\infty} E^{(-2k-1)}_{jj}u^{(-2k-1)}_j} | expression | |
\{\gamma ^{\mu },\gamma ^{\nu }\}=2g^{\mu \upsilon }, \label{Dirac} | expression | |
α
αΌα ααααααΆα | khmer | |
\label{tension}T_{Dp}= \frac{1}{l_s^{p+1} g_s} | expression | |
%V(x) = \frac{3}{4}\frac{1}{\cos^2 x}-\frac{1}{4}.%\label{potential}% | expression | |
S_{ij}(i\pi -\theta )=S_{ij}(h\theta _{h}+H\theta _{H}-\theta)=\prod\limits_{x=1}^{h}\prod\limits_{y=1}^{H}\left\{ x+h,y+H\right\}_{\theta }^{-\mu _{ij}(x+h,y+H)}\,\,. \label{133} | expression | |
αα αααααΈ | khmer | |
ααα αα»ααα ααααα | khmer | |
C(r)=\ln(2\sqrt{2\pi}e^{\gamma +1} r)\quad . \label{l3} | expression | |
\omega_\xi(X,Y)=\langle[X,Y],\xi\rangle=-\langle Y,[X,\xi]\rangle | expression | |
αααα ααα»ααα αα»α ααα αα
ααΎ αααααΆαα αα ααΊ ααΆα
α ααΈ αααααΆαα ααα ααΆα | khmer | |
\bar\delta S^{(2)}=\int_{t_0}^tdt\int dx\,\epsilon^{\mu\nu}\frac{\epsilon^{\rho\lambda}}{\sqrt{-g}}\,D_\rho\partial_\mu\phi\,\bar\delta\bigl(D_\lambda\partial_\nu\phi\bigr)\,,\label{4.2} | expression | |
see you can't get her out | khmer | |
\sum_{\pi(1,2,...n)} \mbox{Tr}\Big[\tau^{(l_0)} \tau^{(l_{\pi(1)})} .....\tau^{(l_{\pi(n)})} \Big]\frac{1}{\tilde{x}_0 - \tilde{x}_{\pi(1)}}\frac{1}{\tilde{x}_{\pi(1)} - \tilde{x}_{\pi(2)}} .....\frac{1}{\tilde{x}_{\pi(n)} - \tilde{x}_0} \; , | expression | |
ααααα | khmer | |
\beta F = - \frac{N}{\beta^3 } \int d \theta d \phi \int_{r_+ + h}^L dr \frac{\sqrt{g_4}}{ ( - g^{'}_{tt } )^2 } = - N \int_0^\beta d \tau \int d \theta d \phi \int_{r_+ + h}^L dr \sqrt{g_4} \frac{1}{ \beta_{local}^4}, \label{free} | expression | |
\delta \phi = \delta \phi_0 + \delta \phi_{-} t^{-1}, | expression | |
\begin{array}{rcl}\omega(\lambda)\wedge\omega(\lambda) & = & 0 \,, \\d \omega(\lambda) & = & 0 \,.\end{array} | expression | |
ααααΆααααΈ | khmer | |
\label{ctildeocho}\begin{array}{rcl}{\tilde C}^{(8)\prime}_{\mu_1\dots\mu_7 z}&=&(i_k N^{(8)})_{\mu_1\dots\mu_7}+7(i_k N^{(7)})_{[\mu_1\dots\mu_6}(C^{(1)}_{\mu_7]}-C^{(1)}_z \frac{g_{z\mu_7]}}{g_{zz}})\\& & \\& & +35(C^{(3)}_{[\mu_1\dots\mu_3}-3C^{(3)}_{[\mu_1\mu_2 z}\frac{g_{z\mu_3}}{g_{zz}})C^{(3)}_{\mu_4\mu_5 z}C^{(... | expression | |
\frac{\delta ^{P}I[\phi +\psi ]}{\delta \eta } | expression | |
αα½α ααα α’ααααΎα ααααΆα αααα α’ααα ααΆα α
ααααααΉα αα ααααΎααΆ ααΈααααΉααααΆ | khmer | |
αα·α ααααα α’αΆαααΈα α | khmer | |
αα―ααα½αααααα
αα»ααΆαααααααΆ | khmer | |
ααα ααΉα | khmer | |
αααΌα | khmer | |
E_C^{(2)\;reg}(R\to\infty,\Lambda)=-\frac{\Lambda}{2\pi}\ln\left[\sinh\left(R\sqrt{\Lambda^2+\omega_0^2}\right)\right]+\frac{1}{2\pi}\int\limits_{0}^{\Lambda}dy\left(R\sqrt{y^2+\omega_0^2}-\ln 2\right)-\frac{\omega_0^2}{4}.\label{b3.17} | expression | |
αα
αααααααΆαααααΌαααΎα | khmer | |
S= \int dt d^2x\left\{\mbox{ Tr }(2Kg^{-1}\dot g)-\frac{\kappa}{2}\epsilon^{ij}A^A_i \dot A^A_j-{\cal H}+A_0^AG^A\right\} | expression | |
\lambda tK_{\left| n\right| }(\mu t)I_{\left| n\right| }(\mu t)q_{-i}q_i.\label{dh} | expression | |
αααΆαα½αααΆααααΆα | khmer | |
I_{\mu}^{\ \nu}\equiv \left[ \delta_\mu^\nu + \phi^{-1}\phi_{\mu\alpha}h^{\alpha\nu}\right] \;,\quad I^{-1}\ _\mu^{\ \alpha} I_\alpha^{\ \nu} =\delta_\mu^\nu \;,\quad I\equiv detI_\mu^{\ \nu}\; . \label{defI} | expression | |
ααΎαααΎα | khmer | |
\label{hyper1}(1+z)(1-z) \frac{d^2}{dz^2} u(z) + \left( (c-2)z + c -2a -2b \right)\frac{d}{dz}u(z) + \frac{2ab}{1+z} = 0, | expression | |
\eta_{11}= - {4\Gamma(d-2) \over \Gamma(2-{d \over 2})\Gamma({d \over 2}-1)\Gamma({d \over 2}-2)\Gamma({d \over 2}+1)}, | expression | |
ααααΆαα αα·α ααΈαα»α | khmer | |
f_{\rm em}=-{\pi^2\over 240}{1\over a^4}.\label{casimirclassic} | expression | |
αα»ααΆααΈ | khmer | |
ααααα
αααααΆααΌα
ααααα
? | khmer | |
ααααΆα ααααα ααααα ααΊ ααααΆα | khmer | |
ααΆ ααα ααΆαα αα
ααααα | khmer | |
ααααα ααααΆααα
α»α | khmer | |
\Psi(\theta)= \left( \begin{array}{lr} \psi_{n,m-1}(\theta) \\ \psi_{n,m}(\theta) \\ \psi_{n,m-1}(\theta) \\ \psi_{n,m}(\theta) \\ \,\,\,\,\,\,\,\vdots\\ \psi_{n,m-1}(\theta) \\ \end{array} \right)_{(2k+1) \times 1} | expression | |
ααΎααααΈααΆααααα | khmer | |
N=T^a \mbox{\tiny $\wedge$} T_a - R_{ab}\mbox{\tiny $\wedge$}e^a\mbox{\tiny $\wedge$} e^b.\label{NY} | expression | |
αααααα αααα·α αα·α ααααααα αα ααΆααααααΌα | khmer | |
{\cal L}_{\rm hyp.kin.} \rightarrow {\cal L}_{\rm hyp.kin.} - \frac32 \sigma'' \phi^*_i \phi^i. | expression | |
α’αα»αααα | khmer | |
comewithalockerwherewecan | khmer | |
\left\{ A,B\right\} _{{\footnotesize PB}}=\sum_{i}\frac{\partial\left(A,B\right) }{\partial\left( x_{i},p_{i}\right) }=-\left\{ B,A\right\}_{{\footnotesize PB}}\;. | expression | |
Was it possible that men | khmer | |
\{C^a,g,\Theta_{\mu},\partial_{\mu}\Theta_{\nu},\ldots\}, | expression | |
ααΆααα»α(αααααΆαα·αααα· | khmer | |
ααααΆαααα ααΆ ααα α
αα ααΈ α’αΆααααα | khmer | |
αααα | khmer | |
αααααα ααααΎ αααΆαα· ( ααααΆ ααΌα ααααααα·ααΆ ααααααα ααΆααΎα )ααΆαααα
αα α’αΆαααα αα ααααΌα | khmer | |
t_2 \frac{t_0^4}{4!}+ 2 \frac{t_1^2}{2!} \frac{t_0^3}{3!} | expression | |
[\frac{1}{u^{3}}\partial _{u}(u^{3}\partial _{u})-\frac{Nk^{2}}{u^{2}}-k'^{2}-\frac{l(l+2)}{u^{2}}]\tilde{\varphi }(u)=0 | expression | |
\hat{K}=\left(\begin{array}{ccc} \frac{B}{4} \delta^{\mu \nu \alpha \beta} & 0 & 0\\ 0 & -\frac{B}{16} & -\frac{B_1}{4} \\ 0 & -\frac{B_1}{4} & \frac{B_1^2}{2B} -A\end{array}\right) | expression |
End of preview. Expand in Data Studio
Synthetic Khmer Math OCR Dataset
Large-scale OCR dataset for Khmer text and LaTeX math expression recognition, generated from synthetic document images. This is the full training set with 146,914 cropped text regions.
Dataset Summary
| Split | Samples | Khmer | LaTeX |
|---|---|---|---|
| train | 117,541 | 50,484 | 67,057 |
| validation | 29,373 | 12,568 | 16,805 |
| Total | 146,914 | 63,052 | 83,862 |
Features
| Feature | Type | Description |
|---|---|---|
image |
PIL Image | Cropped text region from synthetic document |
text |
string | Ground truth text (Khmer or LaTeX source code) |
class |
string | "khmer" or "expression" |
Classes
| ID | Name | Count | Description |
|---|---|---|---|
| 0 | khmer |
63,052 | Khmer script text (books, newspapers, conversations, poetry) |
| 1 | expression |
83,862 | LaTeX math formulas (integrals, matrices, physics equations) |
Examples
Khmer:
- ααΎαααααααααααααααααΌαααααα
- αααααααααααα· αα α αααΆαα
- ααΆα αα αα αααααα ααααα»ααΆ
LaTeX:
\rho^2 \ln(\Lambda l)^2 \ll \frac{1}{l^2} \ln\frac{1}{(\rho l)^2}\tilde{F}(y)= \int_0^{\infty}dx\ln\left(1+\frac{\sin^2xy}{(e^x-\cos x)^2}\right)\hat{K}=\left(\begin{array}{ccc} \frac{B}{4} \delta^{\mu \nu \alpha \beta} & 0 & 0\\ 0 & -\frac{B}{16} & -\frac{B_1}{4} \\ 0 & -\frac{B_1}{4} & \frac{B_1^2}{2B} -A\end{array}\right)
Usage
from datasets import load_dataset
ds = load_dataset("krotreaksmey/synthetic_khmer_math")
# View a sample
example = ds["train"][0]
print(f"Class: {example['class']}")
print(f"Text: {example['text']}")
example["image"]
# Filter by class
khmer_only = ds["train"].filter(lambda x: x["class"] == "khmer")
expression_only = ds["train"].filter(lambda x: x["class"] == "expression")
Image Stats
- Width: 60β1,046 px (avg ~380 px)
- Height: 38β171 px (avg ~74 px)
- Format: PNG with transparency
Generation Pipeline
- Text collection β 62,680 Khmer texts from local books + 83,884 LaTeX formulas from arXiv
- LaTeX rendering β LuaLaTeX + HarfBuzz for proper Khmer Unicode shaping
- Page composition β Random placement on colored backgrounds (in-memory, 35-40 pages/sec)
- YOLOv8 OBB detection β Trained model detects text regions with oriented bounding boxes
- Crop + match β Detection regions cropped and matched to ground truth OCR labels via IoU
Related Datasets
krotreaksmey/khmer_mathβ Smaller curated subset (10,499 samples)krotreaksmey/Yolo_Detect_khmer_mathβ Trained YOLOv8 OBB model
Citation
@misc{synthetic_khmer_math_ocr_2026,
title={Synthetic Khmer Math OCR Dataset},
author={krotreaksmey},
year={2026},
url={https://huggingface.co/datasets/krotreaksmey/synthetic_khmer_math}
}
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