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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-OCRv3_mobile_det \
3 -i https://cdn-uploads.huggingface.co/production/uploads/681c1ecd9539bdde5ae1733c/3ul2Rq4Sk5Cn-l69D695U.png1from paddleocr import TextDetection
2model = TextDetection(model_name="PP-OCRv3_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([[[ 637, 1429],
2 ...,
3 [ 634, 1450]],
4
5 ...,
6
7 [[ 356, 106],
8 ...,
9 [ 356, 127]]], dtype=int16), 'dt_scores': [0.8440782190003071, 0.7211973560197601, ..., 0.9473868156887905]}}
1paddleocr ocr -i https://cdn-uploads.huggingface.co/production/uploads/681c1ecd9539bdde5ae1733c/3ul2Rq4Sk5Cn-l69D695U.png \
2 --text_detection_model_name PP-OCRv3_mobile_det \
3 --text_recognition_model_name PP-OCRv3_mobile_rec \
4 --use_doc_orientation_classify False \
5 --use_doc_unwarping False \
6 --use_textline_orientation False \
7 --save_path ./output \
8 --device gpu:0 1{'res': {'input_path': '/root/.paddlex/predict_input/3ul2Rq4Sk5Cn-l69D695U.png', 'page_index': None, 'model_settings': {'use_doc_preprocessor': True, 'use_textline_orientation': False}, '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([[[ 354, 106],
2 ...,
3 [ 354, 127]],
4
5 ...,
6
7 [[ 633, 1433],
8 ...,
9 [ 633, 1449]]], 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([-1, ..., -1]), 'text_rec_score_thresh': 0.0, 'rec_texts': ['Algorithms for the Markov Entropy Decomposition', 'Andrew J.Ferris and David Poulin', 'Departement de Physique, Universite de Sherbrooke,Quebec, JIK 2RI, 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 aminimization problem with a preconditioned', '09', "Newton's algorithm, aswell ashowtoextractglobal susceptibilities and thermal responses.Wedemonstrate", 'thepower of the method withthe spin-1/2XXZmodel on the 2D square lattice, including the extraction of', 'criticalpointsanddetailsofeachphase.Althoughthemethodsharessomequalitativesimilaritieswithexact-', 'diagonalization, we show theMEDisbothmore accurate and significantlymoreflexible.', 'PACS numbers: 05.10.a, 02.50.Ng, 03.67.a, 74.40.Kb', 'I.INTRODUCTION', 'This approximation becomes exact in the case of a1D quan-', 'tum (or classical) Markov chain [1O], and leads to an expo-', '[', 'Although the equations governing quantum many-body', 'nential reduction of costforexactentropy calculationswhen', 'systemsare simpleto write down,finding solutions for the', 'theglobaldensitymatrixis ahigher-dimensional Markovnet-', 'majority of systems remains incrediblydifficult.Modern', 'work state[12, 13].', 'physics finds itself in need of new tools to compute the emer-', 'The second approximation used in theMED approach is', 'gent behavior of large, many-body systems.', 'related to the N-representibilityproblem.Givena set of lo-', 'There has been a great variety of tools developed to tackle', 'cal but overlapping reduced density matrices fp:f, it is a very', 'many-bodyproblems,butingeneral,large2Dand3Dquan-', 'challengingproblem to determine if there exists aglobal 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 p. This problem is QMA-hard (the', 'notusuallyexpected.Directnumerical diagonalizationcanbe', 'quantumanalogue of NP)[14,15],and is hopelessly diffi-', 'performed for relatively small systemshowever the emer-', 'culttoenforce.Thus,thesecondapproximationemployed', 'gentbehavior of a system in thethermodynamic limitmaybe', 'involves ignoringglobal consistency withapositive opera-', 'difficult to extract, especially in systems with large correlation', 'tor,whilerequiringlocalconsistencyonanyoverlappingre-', 'lengths.MonteCarlo approaches aretechnically exact (up to', 'gions between the pi. At the zero-temperature limit, the MED', '', 'sampling error),but sufferfrom the so-called sign problem', 'approach becomes analogous tothe variational nth-order re-', '一', 'forfermionic,frustrated,or dynamicalproblems.Thus we are', 'duced density matrix approach, where positivity is enforced', '', 'limited to search for clever approximations to solve the ma-', 'onallreduceddensitymatricesofsizen[16-18].', 'jorityofmany-bodyproblems.', 'The MED approachis an extremely flexible cluster method,', 'Over the past century,hundreds of such approximations', 'applicabletobothtranslationally invariant systems of anydi-', 'have been proposed, and we will mention just a few notable', 'mensioninthethermodynamiclimit,aswell asfinite systems', '1', 'examples applicable to quantumlattice models.Mean-field', 'or systems without translational invariance (e.g. disordered', 'theory is simple and frequently arrives at the correct quali-', 'lattices,orharmonicallytrapped atoms in optical lattices)', '11', 'tativedescription,butoftenfails when correlations areim-', 'Thefree energy given byMED is guaranteed to lowerbound', 'portant.Density-matrix renormalisation group (DMRG) [1]', 'the true free energy, which in turn lower-bounds the ground', '[ :A!', '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.', '!XIe', 'size in two- or higher-dimensions [2, 3].Related tensor-', 'The ability to provide a rigorous ground-state energy window', 'networktechniquesdesignedfor2Dsystemsarestillintheir', 'is a powerful validation tool, creating a very compellingrea-', 'infancy[4-6].Series-expansionmethods[7]canbe 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]', 'applicationsto 2D quantumlatticemodels in thethermody-', 'and density-matrix embedding [9].', 'namiclimit.In Sec.II,we give a brief derivation of the', 'Herewediscusstheso-calledMarkoventropydecompo-', 'Markov entropydecomposition.SectionIIIoutlinesarobust', 'sition (MED),recently proposed by Poulin & Hastings [1O]', 'numerical strategy for optimizing the clusters that make up', '(andanalogoustoaslightlyearlierclassicalalgorithm[11)).', 'thedecomposition.InSec.IVweshowhowwecanextend', 'This is a self-consistent cluster method for finitetemperature', 'these algorithms toextractnon-trivial information,such as', 'systemsthattakesadvantageofanapproximationofthe(von', 'specific heat and susceptibilities. We present an application of', 'Neumann) entropy. In [1o], it was shown that the entropy', 'the method to the spin-1/2 XXZ model on a 2D square lattice', 'persitecanberigorouslyupperboundedusingonlylocalin-', 'inSec.V,describinghowtocharacterizethephasediagram', 'formationa local,reduced densitymatrix onN sites,say.', 'anddeterminecriticalpoints,beforeconcludinginSec.Vl'], 'rec_scores': array([0.92904288, ..., 0.92923349]), 'rec_polys': array([[[ 354, 106],
10 ...,
11 [ 354, 127]],
12
13 ...,
14
15 [[ 633, 1433],
16 ...,
17 [ 633, 1449]]], dtype=int16), 'rec_boxes': array([[ 354, ..., 128],
18 ...,
19 [ 633, ..., 1449]], dtype=int16)}}save_path. The visualization output is shown below:
1from paddleocr import PaddleOCR
2
3ocr = PaddleOCR(
4 text_detection_model_name="PP-OCRv3_mobile_det",
5 text_recognition_model_name="PP-OCRv3_mobile_rec",
6 use_doc_orientation_classify=False, # Disables document orientation classification model via this parameter
7 use_doc_unwarping=False, # Disables text image rectification model via this parameter
8 use_textline_orientation=False, # Disables text line orientation classification model via this parameter
9)
10result = ocr.predict("./3ul2Rq4Sk5Cn-l69D695U.png")
11for res in result:
12 res.print()
13 res.save_to_img("output")
14 res.save_to_json("output")