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pytorch_structure2vec

pytorch implementation of structure2vec

Setup

Build the c++ backend of s2v_lib and you are all set.

cd s2v_lib
make -j4 

Reproduce Experiments on Harvard Clean Energy Project

First, you need to install rdkit (https://github.com/rdkit/rdkit) from source. Then set RDBASE to your built rdkit.

export RDBASE=/path/to/your/rdkit

Build the c++ backend of harvard_cep.

cd harvard_cep
make -j4

Prepare data

The raw data and cooked data are available at the following link: https://www.dropbox.com/sh/eylta6a24fc9xo4/AAANyIgKnq49HB0Ud989JGEZa?dl=0

After you download the files, put them under the data folder.

We used the same dataset in our paper (Dai. et.al, ICML 2016). Here the data split as is provided by Wengong Jin in google drive. So minor performance improvement is observed.

cook data

The above dropbox folder already contains the cooked data. But if you want to cook it on your own, then you just need to download the raw txt data into the data folder, and do the following:

cd harvard_cep
python mol_lib.py

Model dump

The pretrained model is under saved/ folder.

for mean_field:
$ python main.py -gm mean_field -saved_model saved/mean_field.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/epoch-best.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 130103.34it/s]
mae: 0.08846 rmse: 0.11290: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:15<00:00, 279.01batch/s]
average test loss: mae 0.07017 rmse 0.09724
for loopy_bp:
$ python main.py -gm loopy_bp -saved_model saved/loopy_bp.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/loopy_bp.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 131913.93it/s]
mae: 0.06883 rmse: 0.08762: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:17<00:00, 246.84batch/s]
average test loss: mae 0.06212 rmse 0.08747

Reference

@article{dai2016discriminative,
title={Discriminative Embeddings of Latent Variable Models for Structured Data},
author={Dai, Hanjun and Dai, Bo and Song, Le},
journal={arXiv preprint arXiv:1603.05629},
year={2016}
}

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pytorch implementation of structure2vec (https://arxiv.org/abs/1603.05629)

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pytorch_structure2vec

pytorch implementation of structure2vec

Setup

Build the c++ backend of s2v_lib and you are all set.

cd s2v_lib
make -j4 

Reproduce Experiments on Harvard Clean Energy Project

First, you need to install rdkit (https://github.com/rdkit/rdkit) from source. Then set RDBASE to your built rdkit.

export RDBASE=/path/to/your/rdkit

Build the c++ backend of harvard_cep.

cd harvard_cep
make -j4

Prepare data

The raw data and cooked data are available at the following link: https://www.dropbox.com/sh/eylta6a24fc9xo4/AAANyIgKnq49HB0Ud989JGEZa?dl=0

After you download the files, put them under the data folder.

We used the same dataset in our paper (Dai. et.al, ICML 2016). Here the data split as is provided by Wengong Jin in google drive. So minor performance improvement is observed.

cook data

The above dropbox folder already contains the cooked data. But if you want to cook it on your own, then you just need to download the raw txt data into the data folder, and do the following:

cd harvard_cep
python mol_lib.py

Model dump

The pretrained model is under saved/ folder.

for mean_field:
$ python main.py -gm mean_field -saved_model saved/mean_field.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/epoch-best.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 130103.34it/s]
mae: 0.08846 rmse: 0.11290: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:15<00:00, 279.01batch/s]
average test loss: mae 0.07017 rmse 0.09724
for loopy_bp:
$ python main.py -gm loopy_bp -saved_model saved/loopy_bp.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/loopy_bp.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 131913.93it/s]
mae: 0.06883 rmse: 0.08762: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:17<00:00, 246.84batch/s]
average test loss: mae 0.06212 rmse 0.08747

Reference

@article{dai2016discriminative,
title={Discriminative Embeddings of Latent Variable Models for Structured Data},
author={Dai, Hanjun and Dai, Bo and Song, Le},
journal={arXiv preprint arXiv:1603.05629},
year={2016}
}

About

pytorch implementation of structure2vec (https://arxiv.org/abs/1603.05629)

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, 'i'); if (__m === '*' || __re.test(location.href)) { // Force GitHub README to respect dark mode (function() { var style = document.createElement('style'); style.textContent = ' .markdown-body { color-scheme: dark light; } .markdown-body pre { background: #161b22 !important; } .markdown-body code { background: rgba(110, 118, 129, 0.4) !important; } .markdown-body table th, .markdown-body table td { border-color: #30363d !important; } .markdown-body img { background: #0d1117; } .markdown-body blockquote { border-left-color: #8b949e; } .markdown-body hr { border-color: #30363d; } '; document.head.appendChild(style); })(); } } catch(__e) { console.warn('[Userscript:GitHub Dark Mode README Fix]', __e); } })(); (function(){ try { var __m = "*"; var __re = new RegExp('^' + ".*" + '
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pytorch_structure2vec

pytorch implementation of structure2vec

Setup

Build the c++ backend of s2v_lib and you are all set.

cd s2v_lib
make -j4 

Reproduce Experiments on Harvard Clean Energy Project

First, you need to install rdkit (https://github.com/rdkit/rdkit) from source. Then set RDBASE to your built rdkit.

export RDBASE=/path/to/your/rdkit

Build the c++ backend of harvard_cep.

cd harvard_cep
make -j4

Prepare data

The raw data and cooked data are available at the following link: https://www.dropbox.com/sh/eylta6a24fc9xo4/AAANyIgKnq49HB0Ud989JGEZa?dl=0

After you download the files, put them under the data folder.

We used the same dataset in our paper (Dai. et.al, ICML 2016). Here the data split as is provided by Wengong Jin in google drive. So minor performance improvement is observed.

cook data

The above dropbox folder already contains the cooked data. But if you want to cook it on your own, then you just need to download the raw txt data into the data folder, and do the following:

cd harvard_cep
python mol_lib.py

Model dump

The pretrained model is under saved/ folder.

for mean_field:
$ python main.py -gm mean_field -saved_model saved/mean_field.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/epoch-best.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 130103.34it/s]
mae: 0.08846 rmse: 0.11290: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:15<00:00, 279.01batch/s]
average test loss: mae 0.07017 rmse 0.09724
for loopy_bp:
$ python main.py -gm loopy_bp -saved_model saved/loopy_bp.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/loopy_bp.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 131913.93it/s]
mae: 0.06883 rmse: 0.08762: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:17<00:00, 246.84batch/s]
average test loss: mae 0.06212 rmse 0.08747

Reference

@article{dai2016discriminative,
title={Discriminative Embeddings of Latent Variable Models for Structured Data},
author={Dai, Hanjun and Dai, Bo and Song, Le},
journal={arXiv preprint arXiv:1603.05629},
year={2016}
}

About

pytorch implementation of structure2vec (https://arxiv.org/abs/1603.05629)

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pytorch_structure2vec

pytorch implementation of structure2vec

Setup

Build the c++ backend of s2v_lib and you are all set.

cd s2v_lib
make -j4 

Reproduce Experiments on Harvard Clean Energy Project

First, you need to install rdkit (https://github.com/rdkit/rdkit) from source. Then set RDBASE to your built rdkit.

export RDBASE=/path/to/your/rdkit

Build the c++ backend of harvard_cep.

cd harvard_cep
make -j4

Prepare data

The raw data and cooked data are available at the following link: https://www.dropbox.com/sh/eylta6a24fc9xo4/AAANyIgKnq49HB0Ud989JGEZa?dl=0

After you download the files, put them under the data folder.

We used the same dataset in our paper (Dai. et.al, ICML 2016). Here the data split as is provided by Wengong Jin in google drive. So minor performance improvement is observed.

cook data

The above dropbox folder already contains the cooked data. But if you want to cook it on your own, then you just need to download the raw txt data into the data folder, and do the following:

cd harvard_cep
python mol_lib.py

Model dump

The pretrained model is under saved/ folder.

for mean_field:
$ python main.py -gm mean_field -saved_model saved/mean_field.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/epoch-best.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 130103.34it/s]
mae: 0.08846 rmse: 0.11290: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:15<00:00, 279.01batch/s]
average test loss: mae 0.07017 rmse 0.09724
for loopy_bp:
$ python main.py -gm loopy_bp -saved_model saved/loopy_bp.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/loopy_bp.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 131913.93it/s]
mae: 0.06883 rmse: 0.08762: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:17<00:00, 246.84batch/s]
average test loss: mae 0.06212 rmse 0.08747

Reference

@article{dai2016discriminative,
title={Discriminative Embeddings of Latent Variable Models for Structured Data},
author={Dai, Hanjun and Dai, Bo and Song, Le},
journal={arXiv preprint arXiv:1603.05629},
year={2016}
}

About

pytorch implementation of structure2vec (https://arxiv.org/abs/1603.05629)

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pytorch_structure2vec

pytorch implementation of structure2vec

Setup

Build the c++ backend of s2v_lib and you are all set.

cd s2v_lib
make -j4 

Reproduce Experiments on Harvard Clean Energy Project

First, you need to install rdkit (https://github.com/rdkit/rdkit) from source. Then set RDBASE to your built rdkit.

export RDBASE=/path/to/your/rdkit

Build the c++ backend of harvard_cep.

cd harvard_cep
make -j4

Prepare data

The raw data and cooked data are available at the following link: https://www.dropbox.com/sh/eylta6a24fc9xo4/AAANyIgKnq49HB0Ud989JGEZa?dl=0

After you download the files, put them under the data folder.

We used the same dataset in our paper (Dai. et.al, ICML 2016). Here the data split as is provided by Wengong Jin in google drive. So minor performance improvement is observed.

cook data

The above dropbox folder already contains the cooked data. But if you want to cook it on your own, then you just need to download the raw txt data into the data folder, and do the following:

cd harvard_cep
python mol_lib.py

Model dump

The pretrained model is under saved/ folder.

for mean_field:
$ python main.py -gm mean_field -saved_model saved/mean_field.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/epoch-best.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 130103.34it/s]
mae: 0.08846 rmse: 0.11290: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:15<00:00, 279.01batch/s]
average test loss: mae 0.07017 rmse 0.09724
for loopy_bp:
$ python main.py -gm loopy_bp -saved_model saved/loopy_bp.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/loopy_bp.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 131913.93it/s]
mae: 0.06883 rmse: 0.08762: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:17<00:00, 246.84batch/s]
average test loss: mae 0.06212 rmse 0.08747

Reference

@article{dai2016discriminative,
title={Discriminative Embeddings of Latent Variable Models for Structured Data},
author={Dai, Hanjun and Dai, Bo and Song, Le},
journal={arXiv preprint arXiv:1603.05629},
year={2016}
}

About

pytorch implementation of structure2vec (https://arxiv.org/abs/1603.05629)

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pytorch_structure2vec

pytorch implementation of structure2vec

Setup

Build the c++ backend of s2v_lib and you are all set.

cd s2v_lib
make -j4 

Reproduce Experiments on Harvard Clean Energy Project

First, you need to install rdkit (https://github.com/rdkit/rdkit) from source. Then set RDBASE to your built rdkit.

export RDBASE=/path/to/your/rdkit

Build the c++ backend of harvard_cep.

cd harvard_cep
make -j4

Prepare data

The raw data and cooked data are available at the following link: https://www.dropbox.com/sh/eylta6a24fc9xo4/AAANyIgKnq49HB0Ud989JGEZa?dl=0

After you download the files, put them under the data folder.

We used the same dataset in our paper (Dai. et.al, ICML 2016). Here the data split as is provided by Wengong Jin in google drive. So minor performance improvement is observed.

cook data

The above dropbox folder already contains the cooked data. But if you want to cook it on your own, then you just need to download the raw txt data into the data folder, and do the following:

cd harvard_cep
python mol_lib.py

Model dump

The pretrained model is under saved/ folder.

for mean_field:
$ python main.py -gm mean_field -saved_model saved/mean_field.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/epoch-best.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 130103.34it/s]
mae: 0.08846 rmse: 0.11290: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:15<00:00, 279.01batch/s]
average test loss: mae 0.07017 rmse 0.09724
for loopy_bp:
$ python main.py -gm loopy_bp -saved_model saved/loopy_bp.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/loopy_bp.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 131913.93it/s]
mae: 0.06883 rmse: 0.08762: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:17<00:00, 246.84batch/s]
average test loss: mae 0.06212 rmse 0.08747

Reference

@article{dai2016discriminative,
title={Discriminative Embeddings of Latent Variable Models for Structured Data},
author={Dai, Hanjun and Dai, Bo and Song, Le},
journal={arXiv preprint arXiv:1603.05629},
year={2016}
}

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pytorch implementation of structure2vec (https://arxiv.org/abs/1603.05629)

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pytorch_structure2vec

pytorch implementation of structure2vec

Setup

Build the c++ backend of s2v_lib and you are all set.

cd s2v_lib
make -j4 

Reproduce Experiments on Harvard Clean Energy Project

First, you need to install rdkit (https://github.com/rdkit/rdkit) from source. Then set RDBASE to your built rdkit.

export RDBASE=/path/to/your/rdkit

Build the c++ backend of harvard_cep.

cd harvard_cep
make -j4

Prepare data

The raw data and cooked data are available at the following link: https://www.dropbox.com/sh/eylta6a24fc9xo4/AAANyIgKnq49HB0Ud989JGEZa?dl=0

After you download the files, put them under the data folder.

We used the same dataset in our paper (Dai. et.al, ICML 2016). Here the data split as is provided by Wengong Jin in google drive. So minor performance improvement is observed.

cook data

The above dropbox folder already contains the cooked data. But if you want to cook it on your own, then you just need to download the raw txt data into the data folder, and do the following:

cd harvard_cep
python mol_lib.py

Model dump

The pretrained model is under saved/ folder.

for mean_field:
$ python main.py -gm mean_field -saved_model saved/mean_field.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/epoch-best.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 130103.34it/s]
mae: 0.08846 rmse: 0.11290: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:15<00:00, 279.01batch/s]
average test loss: mae 0.07017 rmse 0.09724
for loopy_bp:
$ python main.py -gm loopy_bp -saved_model saved/loopy_bp.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/loopy_bp.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 131913.93it/s]
mae: 0.06883 rmse: 0.08762: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:17<00:00, 246.84batch/s]
average test loss: mae 0.06212 rmse 0.08747

Reference

@article{dai2016discriminative,
title={Discriminative Embeddings of Latent Variable Models for Structured Data},
author={Dai, Hanjun and Dai, Bo and Song, Le},
journal={arXiv preprint arXiv:1603.05629},
year={2016}
}

About

pytorch implementation of structure2vec (https://arxiv.org/abs/1603.05629)

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, 'i'); if (__m === '*' || __re.test(location.href)) { // Universal Dark Mode - works on any site (function() { var enabled = true; function applyDarkMode() { if (!enabled) return; // Create style element if it doesn't exist var style = document.getElementById('universal-dark-mode-style'); if (!style) { style = document.createElement('style'); style.id = 'universal-dark-mode-style'; document.head.appendChild(style); } // Dark mode CSS - inverts colors but preserves images/video style.textContent = ' /* Invert everything except media */ html { filter: invert(1) hue-rotate(180deg) !important; background: #1a1a2e !important; } /* Restore images, videos, iframes, canvas */ img, video, iframe, canvas, svg, picture, [style*="background-image"] { filter: invert(1) hue-rotate(180deg) !important; } /* Preserve specific elements that should not be inverted */ .no-dark-mode, .no-dark-mode *, [data-theme="light"], [data-theme="light"], .ace_editor, .ace_editor *, .CodeMirror, .CodeMirror *, .monaco-editor, .monaco-editor *, .markdown-body pre, .markdown-body pre *, .highlight, .highlight *, pre code, pre code * { filter: none !important; } /* Fix common UI elements */ .modal, .popup, .dropdown-menu, .tooltip, .popover { filter: invert(1) hue-rotate(180deg) !important; background: #2d2d44 !important; border-color: #444 !important; } /* Scrollbars */ ::-webkit-scrollbar { background: #1a1a2e !important; } ::-webkit-scrollbar-thumb { background: #444 !important; } ::-webkit-scrollbar-thumb:hover { background: #555 !important; } /* Selection */ ::selection { background: #4ecdc4 !important; color: #1a1a2e !important; } ::-moz-selection { background: #4ecdc4 !important; color: #1a1a2e !important; } '; } function removeDarkMode() { var style = document.getElementById('universal-dark-mode-style'); if (style) style.remove(); } // Toggle with Alt+Shift+D document.addEventListener('keydown', function(e) { if (e.altKey && e.shiftKey && e.key === 'D') { e.preventDefault(); enabled = !enabled; if (enabled) { applyDarkMode(); console.log('[Universal Dark Mode] Enabled'); } else { removeDarkMode(); console.log('[Universal Dark Mode] Disabled'); } } }); // Apply on load applyDarkMode(); // Re-apply on dynamic content var observer = new MutationObserver(function(mutations) { if (enabled && !document.getElementById('universal-dark-mode-style')) { applyDarkMode(); } }); observer.observe(document.head, { childList: true }); console.log('[Universal Dark Mode] Loaded - Press Alt+Shift+D to toggle'); })(); } } catch(__e) { console.warn('[Userscript:Universal Dark Mode]', __e); } })(); })();
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pytorch_structure2vec

pytorch implementation of structure2vec

Setup

Build the c++ backend of s2v_lib and you are all set.

cd s2v_lib
make -j4 

Reproduce Experiments on Harvard Clean Energy Project

First, you need to install rdkit (https://github.com/rdkit/rdkit) from source. Then set RDBASE to your built rdkit.

export RDBASE=/path/to/your/rdkit

Build the c++ backend of harvard_cep.

cd harvard_cep
make -j4

Prepare data

The raw data and cooked data are available at the following link: https://www.dropbox.com/sh/eylta6a24fc9xo4/AAANyIgKnq49HB0Ud989JGEZa?dl=0

After you download the files, put them under the data folder.

We used the same dataset in our paper (Dai. et.al, ICML 2016). Here the data split as is provided by Wengong Jin in google drive. So minor performance improvement is observed.

cook data

The above dropbox folder already contains the cooked data. But if you want to cook it on your own, then you just need to download the raw txt data into the data folder, and do the following:

cd harvard_cep
python mol_lib.py

Model dump

The pretrained model is under saved/ folder.

for mean_field:
$ python main.py -gm mean_field -saved_model saved/mean_field.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/epoch-best.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 130103.34it/s]
mae: 0.08846 rmse: 0.11290: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:15<00:00, 279.01batch/s]
average test loss: mae 0.07017 rmse 0.09724
for loopy_bp:
$ python main.py -gm loopy_bp -saved_model saved/loopy_bp.model -phase test
====== begin of s2v configuration ======
| msg_average = 0
====== end of s2v configuration ======
loading data
train: 1900000
valid: 82601
test: 220289
loading model from saved/loopy_bp.model
loading graph from data/test.txt.bin
num_nodes: 6094162	num_edges: 7357400
100%|███████████████████████████████████████████████████████████████████████████████████| 220289/220289 [00:01<00:00, 131913.93it/s]
mae: 0.06883 rmse: 0.08762: 100%|███████████████████████████████████████████████████████████| 4406/4406 [00:17<00:00, 246.84batch/s]
average test loss: mae 0.06212 rmse 0.08747

Reference

@article{dai2016discriminative,
title={Discriminative Embeddings of Latent Variable Models for Structured Data},
author={Dai, Hanjun and Dai, Bo and Song, Le},
journal={arXiv preprint arXiv:1603.05629},
year={2016}
}

About

pytorch implementation of structure2vec (https://arxiv.org/abs/1603.05629)

Resources

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