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| Handwritten Chinese | Handwritten English | Printed Chinese | Printed English | Traditional Chinese | Ancient Text | Japanese | General Scenario | Pinyin | Rotation | Distortion | Artistic Text | Average |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| 0.744 | 0.777 | 0.905 | 0.910 | 0.823 | 0.581 | 0.727 | 0.721 | 0.575 | 0.647 | 0.827 | 0.525 | 0.770 |
1# for CUDA11.8
2python -m pip install paddlepaddle-gpu==3.0.0 -i https://www.paddlepaddle.org.cn/packages/stable/cu118/
3
4# for CUDA12.6
5python -m pip install paddlepaddle-gpu==3.0.0 -i https://www.paddlepaddle.org.cn/packages/stable/cu126/
6
7# for CPU
8python -m pip install paddlepaddle==3.0.0 -i https://www.paddlepaddle.org.cn/packages/stable/cpu/python -m pip install paddleocr1paddleocr text_detection \
2 --model_name PP-OCRv5_mobile_det \
3 -i https://cdn-uploads.huggingface.co/production/uploads/681c1ecd9539bdde5ae1733c/3ul2Rq4Sk5Cn-l69D695U.png1from paddleocr import TextDetection
2model = TextDetection(model_name="PP-OCRv5_mobile_det")
3output = model.predict(input="3ul2Rq4Sk5Cn-l69D695U.png", batch_size=1)
4for res in output:
5 res.print()
6 res.save_to_img(save_path="./output/")
7 res.save_to_json(save_path="./output/res.json")1{'res': {'input_path': '/root/.paddlex/predict_input/3ul2Rq4Sk5Cn-l69D695U.png', 'page_index': None, 'dt_polys': array([[[ 105, 1431],
2 ...,
3 [ 105, 1452]],
4
5 ...,
6
7 [[ 353, 106],
8 ...,
9 [ 353, 129]]], dtype=int16), 'dt_scores': [0.8306416015066644, 0.7603795581201811, ..., 0.8819806867477359]}}1paddleocr ocr -i https://cdn-uploads.huggingface.co/production/uploads/681c1ecd9539bdde5ae1733c/3ul2Rq4Sk5Cn-l69D695U.png \
2 --text_detection_model_name PP-OCRv5_mobile_det \
3 --use_doc_orientation_classify False \
4 --use_doc_unwarping False \
5 --use_textline_orientation True \
6 --save_path ./output \
7 --device gpu:0 1{'res': {'input_path': 'printing_en/3ul2Rq4Sk5Cn-l69D695U.png', 'page_index': None, 'model_settings': {'use_doc_preprocessor': True, 'use_textline_orientation': True}, 'doc_preprocessor_res': {'input_path': None, 'page_index': None, 'model_settings': {'use_doc_orientation_classify': False, 'use_doc_unwarping': False}, 'angle': -1}, 'dt_polys': array([[[ 352, 105],
2 ...,
3 [ 352, 128]],
4
5 ...,
6
7 [[ 632, 1431],
8 ...,
9 [ 632, 1447]]], dtype=int16), 'text_det_params': {'limit_side_len': 64, 'limit_type': 'min', 'thresh': 0.3, 'max_side_limit': 4000, 'box_thresh': 0.6, 'unclip_ratio': 1.5}, 'text_type': 'general', 'textline_orientation_angles': array([0, ..., 0]), 'text_rec_score_thresh': 0.0, 'rec_texts': ['Algorithms for the Markov Entropy Decomposition', 'Andrew J. Ferris and David Poulin', 'Département de Physique, Université de Sherbrooke, Québec, JI K 2R1, Canada', '(Dated: October 31, 2018)', 'The Markov entropy decomposition (MED) is a recently-proposed, cluster-based simulation method for fi -', 'nite temperature quantum systems with arbitrary geometry. In this paper, we detail numerical algorithms for', 'performing the required steps of the MED, principally solving a minimization problem with a preconditioned', 'arXiv:1212.1442v1 [cond-mat.stat-mech] 6 Dec 2012', "Newton's algorithm, as well as how to extract global susceptibilities and thermal responses. We demonstrate", 'the power of the method with the spin-1/2 XXZ model on the 2D square lattice, including the extraction of', 'critical points and details of each phase. Although the method shares some qualitative similarities with exact-', 'diagonalization, we show the MED is both more accurate and significantly more flexible.', 'PACS numbers: 05.10.—a, 02.50.Ng, 03.67.–a, 74.40.Kb', 'I. INTRODUCTION', 'This approximation becomes exact in the case of a 1D quan-', 'tum (or classical) Markov chain [1O], and leads to an expo-', 'Although the equations governing quantum many-body', 'nential reduction of cost for exact entropy calculations when', 'systems are simple to write down, finding solutions for the', 'the global density matrix is a higher-dimensional Markov net-', 'majority of systems remains incredibly difficult. Modern', 'work state [12, 13].', 'physics finds itself in need of new tools to compute the emer-', 'The second approximation used in the MED approach is', 'gent behavior of large, many-body systems.', 'related to the N-representibility problem. Given a set of lo-', 'There has been a great variety of tools developed to tackle', 'cal but overlapping reduced density matrices { ρi }, it is a very', 'many-body problems, but in general, large 2D and 3D quan-', 'challenging problem to determine if there exists a global den.', 'tum systems remain hard to deal with. Most systems are', 'sity operator which is positive semi-definite and whose partial', 'thought to be non-integrable, so exact analytic solutions are', 'trace agrees with each ρi. This problem is QMA-hard (the', 'not usually expected. Direct numerical diagonalization can be', 'quantum analogue of NP) [14, 15], and is hopelessly diffi-', 'performed for relatively small systems — however the emer-', 'cult to enforce. Thus, the second approximation employed', 'gent behavior of a system in the thermodynamic limit may be', 'involves ignoring global consistency with a positive opera-', 'difficult to extract, especially in systems with large correlation', 'tor, while requiring local consistency on any overlapping re-', 'lengths. Monte Carlo approaches are technically exact (up to', 'gions between the ρi. At the zero-temperature limit, the MED', 'sampling error), but suffer from the so-called sign problem', 'approach becomes analogous to the variational nth-order re-', 'for fermionic, frustrated, or dynamical problems. Thus we are', 'duced density matrix approach, where positivity is enforced', 'limited to search for clever approximations to solve the ma-', 'on all reduced density matrices of size n [16–18].', 'jority of many-body problems.', 'The MED approach is an extremely flexible cluster method.', 'Over the past century, hundreds of such approximations', 'applicable to both translationally invariant systems of any di-', 'have been proposed, and we will mention just a few notable', 'mension in the thermodynamic limit, as well as finite systems', 'examples applicable to quantum lattice models. Mean-field', 'or systems without translational invariance (e.g. disordered', 'theory is simple and frequently arrives at the correct quali-', 'lattices, or harmonically trapped atoms in optical lattices).', 'tative description, but often fails when correlations are im-', 'The free energy given by MED is guaranteed to lower bound', 'portant. Density-matrix renormalisation group (DMRG) [1]', 'the true free energy, which in turn lower-bounds the ground', 'is efficient and extremely accurate at solving 1D problems,', 'state energy — thus providing a natural complement to varia-', 'but the computational cost grows exponentially with system', 'tional approaches which upper-bound the ground state energy.', 'size in two- or higher-dimensions [2, 3]. Related tensor-', 'The ability to provide a rigorous ground-state energy window', 'network techniques designed for 2D systems are still in their', 'is a powerful validation tool, creating a very compelling rea-', 'infancy [4–6]. Series-expansion methods [7] can be success-', 'son to use this approach.', 'ful, but may diverge or otherwise converge slowly, obscuring', 'In this paper we paper we present a pedagogical introduc-', 'the state in certain regimes. There exist a variety of cluster-', 'tion to MED, including numerical implementation issues and', 'based techniques, such as dynamical-mean-field theory [8]', 'applications to 2D quantum lattice models in the thermody-', 'and density-matrix embedding [9]', 'namic limit. In Sec. II. we giye a brief deriyation of the', 'Here we discuss the so-called Markov entropy decompo-', 'Markov entropy decomposition. Section III outlines a robust', 'sition (MED), recently proposed by Poulin & Hastings [10]', 'numerical strategy for optimizing the clusters that make up', '(and analogous to a slightly earlier classical algorithm [11]).', 'the decomposition. In Sec. IV we show how we can extend', 'This is a self-consistent cluster method for fi nite temperature', 'these algorithms to extract non-trivial information, such as', 'systems that takes advantage of an approximation of the (von', 'specific heat and susceptibilities. We present an application of', 'Neumann) entropy. In [10], it was shown that the entropy', 'the method to the spin-1/2 XXZ model on a 2D square lattice', 'per site can be rigorously upper bounded using only local in-', 'in Sec. V, describing how to characterize the phase diagram', 'formation — a local, reduced density matrix on N sites, say.', 'and determine critical points, before concluding in Sec. VI.'], 'rec_scores': array([0.99388635, ..., 0.99304372]), 'rec_polys': array([[[ 352, 105],
10 ...,
11 [ 352, 128]],
12
13 ...,
14
15 [[ 632, 1431],
16 ...,
17 [ 632, 1447]]], dtype=int16), 'rec_boxes': array([[ 352, ..., 128],
18 ...,
19 [ 632, ..., 1447]], dtype=int16)}}save_path. The visualization output is shown below:1from paddleocr import PaddleOCR
2
3ocr = PaddleOCR(
4 text_detection_model_name="PP-OCRv5_mobile_det",
5 use_doc_orientation_classify=False, # Use use_doc_orientation_classify to enable/disable document orientation classification model
6 use_doc_unwarping=False, # Use use_doc_unwarping to enable/disable document unwarping module
7 use_textline_orientation=True, # Use use_textline_orientation to enable/disable textline orientation classification model
8 device="gpu:0", # Use device to specify GPU for model inference
9)
10result = ocr.predict("https://cdn-uploads.huggingface.co/production/uploads/681c1ecd9539bdde5ae1733c/3ul2Rq4Sk5Cn-l69D695U.png")
11for res in result:
12 res.print()
13 res.save_to_img("output")
14 res.save_to_json("output")PP-OCRv5_server_det, so it is needed that specifing to PP-OCRv5_mobile_det by argument text_detection_model_name. And you can also use the local model file by argument text_detection_model_dir. For details about usage command and descriptions of parameters, please refer to the Document.1paddleocr pp_structurev3 -i https://cdn-uploads.huggingface.co/production/uploads/681c1ecd9539bdde5ae1733c/mG4tnwfrvECoFMu-S9mxo.png \
2 --text_detection_model_name PP-OCRv5_mobile_det \
3 --use_doc_orientation_classify False \
4 --use_doc_unwarping False \
5 --use_textline_orientation False \
6 --device gpu:0save_path. The predicted markdown visualization is shown below:1from paddleocr import PPStructureV3
2
3pipeline = PPStructureV3(
4 text_detection_model_name="PP-OCRv5_mobile_det",
5 use_doc_orientation_classify=False, # Use use_doc_orientation_classify to enable/disable document orientation classification model
6 use_doc_unwarping=False, # Use use_doc_unwarping to enable/disable document unwarping module
7 use_textline_orientation=False, # Use use_textline_orientation to enable/disable textline orientation classification model
8 device="gpu:0", # Use device to specify GPU for model inference
9 )
10output = pipeline.predict("./pp_structure_v3_demo.png")
11for res in output:
12 res.print() # Print the structured prediction output
13 res.save_to_json(save_path="output") ## Save the current image's structured result in JSON format
14 res.save_to_markdown(save_path="output") ## Save the current image's result in Markdown formatPP-OCRv5_server_det, so it is needed that specifing to PP-OCRv5_mobile_det by argument text_detection_model_name. And you can also use the local model file by argument text_detection_model_dir. For details about usage command and descriptions of parameters, please refer to the Document.