diff --git a/docs/AI/SinglePropertyPrediction/dft_3d_Tc_supercon_hydride.md b/docs/AI/SinglePropertyPrediction/dft_3d_Tc_supercon_hydride.md
new file mode 100644
index 000000000..83d8745df
--- /dev/null
+++ b/docs/AI/SinglePropertyPrediction/dft_3d_Tc_supercon_hydride.md
@@ -0,0 +1,20 @@
+# Model for Superconducting Tc of High Pressure Hydrides
+ - Description: This is a benchmark to evaluate how accurately an AI model can predict the superconducting transition temperature of hydride materials under pressure. The dataset contains the structures and DFT calculated Tc of the hydride materials under various amounts of pressure. Here we use mean absolute error (MAE) to compare models with respect to DFT accuracy. External links: https://iopscience.iop.org/article/10.1088/2752-5724/ad4a94
Reference(s): [https://www.nature.com/articles/s41524-020-00440-1](https://www.nature.com/articles/s41524-020-00440-1), [https://iopscience.iop.org/article/10.1088/2752-5724/ad4a94](https://iopscience.iop.org/article/10.1088/2752-5724/ad4a94), [https://doi.org/10.48550/arXiv.2305.11842](https://doi.org/10.48550/arXiv.2305.11842)
+
+
+Model benchmarks
+
+
\ No newline at end of file
diff --git a/docs/AI/SinglePropertyPrediction/dft_3d_Tc_supercon_hydride_plus_bulk.md b/docs/AI/SinglePropertyPrediction/dft_3d_Tc_supercon_hydride_plus_bulk.md
new file mode 100644
index 000000000..ff5fd7d84
--- /dev/null
+++ b/docs/AI/SinglePropertyPrediction/dft_3d_Tc_supercon_hydride_plus_bulk.md
@@ -0,0 +1,20 @@
+# Model for Superconducting Tc of High Pressure Hydrides
+ - Description: This is a benchmark to evaluate how accurately an AI model can predict the superconducting transition temperature of hydride materials under pressure. The dataset contains the structures and DFT calculated Tc of the hydride materials under various amounts of pressure plus the DFT dataset of bulk hydride materials. Here we use mean absolute error (MAE) to compare models with respect to DFT accuracy. External links: https://iopscience.iop.org/article/10.1088/2752-5724/ad4a95, https://www.nature.com/articles/s41524-022-00933-1
Reference(s): [https://www.nature.com/articles/s41524-020-00440-1](https://www.nature.com/articles/s41524-020-00440-1), [https://iopscience.iop.org/article/10.1088/2752-5724/ad4a94](https://iopscience.iop.org/article/10.1088/2752-5724/ad4a94), [https://doi.org/10.48550/arXiv.2305.11842](https://doi.org/10.48550/arXiv.2305.11842)
+
+
+Model benchmarks
+
+
\ No newline at end of file
diff --git a/jarvis_leaderboard/benchmarks/AI/SinglePropertyPrediction/dft_3d_Tc_supercon_hydride.json.zip b/jarvis_leaderboard/benchmarks/AI/SinglePropertyPrediction/dft_3d_Tc_supercon_hydride.json.zip
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diff --git a/jarvis_leaderboard/benchmarks/AI/SinglePropertyPrediction/dft_3d_Tc_supercon_hydride_plus_bulk.json.zip b/jarvis_leaderboard/benchmarks/AI/SinglePropertyPrediction/dft_3d_Tc_supercon_hydride_plus_bulk.json.zip
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index 000000000..f0e2c5596
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diff --git a/jarvis_leaderboard/benchmarks/benchmark_dois.json b/jarvis_leaderboard/benchmarks/benchmark_dois.json
index 44ca02c68..30489a82c 100644
--- a/jarvis_leaderboard/benchmarks/benchmark_dois.json
+++ b/jarvis_leaderboard/benchmarks/benchmark_dois.json
@@ -203,6 +203,16 @@
"https://www.nature.com/articles/s41524-020-00440-1",
"https://doi.org/10.48550/arXiv.2305.11842"
],
+ "dft_3d_Tc_supercon_hydride.json.zip": [
+ "https://iopscience.iop.org/article/10.1088/2752-5724/ad4a94",
+ "https://www.nature.com/articles/s41524-020-00440-1",
+ "https://doi.org/10.48550/arXiv.2305.11842"
+ ],
+ "dft_3d_Tc_supercon_hydride_plus_bulk.json.zip": [
+ "https://iopscience.iop.org/article/10.1088/2752-5724/ad4a94",
+ "https://www.nature.com/articles/s41524-020-00440-1",
+ "https://doi.org/10.48550/arXiv.2305.11842"
+ ],
"dft_3d_ph_heat_capacity.json.zip": [
"https://www.nature.com/articles/s41524-020-00440-1",
"https://doi.org/10.48550/arXiv.2305.11842"
diff --git a/jarvis_leaderboard/benchmarks/descriptions.csv b/jarvis_leaderboard/benchmarks/descriptions.csv
index 28628e174..3b6bb8662 100644
--- a/jarvis_leaderboard/benchmarks/descriptions.csv
+++ b/jarvis_leaderboard/benchmarks/descriptions.csv
@@ -46,6 +46,8 @@ AI,SinglePropertyPrediction,qm9_std_jctc_U,This is a benchmark to evaluate how a
AI,SinglePropertyPrediction,qm9_std_jctc_U0,This is a benchmark to evaluate how accurately an AI model can predict the internal energy (U0) at 0 K using the QM9 dataset. The dataset contains the structures and properties of molecules. Here we use mean absolute error (MAE) to compare models with respect to DFT accuracy. External links: https://www.nature.com/articles/sdata201422,
AI,SinglePropertyPrediction,qm9_std_jctc_ZPVE,This is a benchmark to evaluate how accurately an AI model can predict the zero-point vibrational energy (ZPVE) using the QM9 dataset. The dataset contains the structures and properties of molecules. Here we use mean absolute error (MAE) to compare models with respect to DFT accuracy. External links: https://www.nature.com/articles/sdata201422,
AI,SinglePropertyPrediction,qm9_std_jctc_alpha,This is a benchmark to evaluate how accurately an AI model can predict the isotropic polarizability using the QM9 dataset. The dataset contains the structures and properties of molecules. Here we use mean absolute error (MAE) to compare models with respect to DFT accuracy. External links: https://www.nature.com/articles/sdata201422,
+AI,SinglePropertyPrediction,dft_3d_Tc_supercon_hydride,This is a benchmark to evaluate how accurately an AI model can predict the superconducting transition temperature of hydride materials under pressure. The dataset contains the structures and DFT calculated Tc of the hydride materials under various amounts of pressure. Here we use mean absolute error (MAE) to compare models with respect to DFT accuracy. External links: https://iopscience.iop.org/article/10.1088/2752-5724/ad4a94,
+AI,SinglePropertyPrediction,dft_3d_Tc_supercon_hydride_plus_bulk,"This is a benchmark to evaluate how accurately an AI model can predict the superconducting transition temperature of hydride materials under pressure. The dataset contains the structures and DFT calculated Tc of the hydride materials under various amounts of pressure plus the DFT dataset of bulk hydride materials. Here we use mean absolute error (MAE) to compare models with respect to DFT accuracy. External links: https://iopscience.iop.org/article/10.1088/2752-5724/ad4a95, https://www.nature.com/articles/s41524-022-00933-1",
AI,SinglePropertyPrediction,dft_3d_avg_elec_mass,This is a benchmark to evaluate how accurately an AI model can predict the average electron mass using the JARVIS-DFT (dft_3d) dataset. The dataset contains different types of chemical formula and atomic structures. Here we use mean absolute error (MAE) to compare models with respect to DFT accuracy.,
AI,SinglePropertyPrediction,dft_3d_avg_hole_mass,This is a benchmark to evaluate how accurately an AI model can predict the average hole mass using the JARVIS-DFT (dft_3d) dataset. The dataset contains different types of chemical formula and atomic structures. Here we use mean absolute error (MAE) to compare models with respect to DFT accuracy.,
AI,SinglePropertyPrediction,qmof_bandgap,This is a benchmark to evaluate how accurately an AI model can predict the bandgap using the QMOF dataset. The dataset contains different types of metal organic frameworks. Here we use mean absolute error (MAE) to compare models with respect to DFT accuracy. External links: https://github.com/Andrew-S-Rosen/QMOF,
@@ -295,4 +297,4 @@ FF,SinglePropertyPrediction,biobench_deltaF,This is a benchmark to evaluate how
FF,SinglePropertyPrediction,biobench_left_handed_population,This is a benchmark to evaluate how accurately an FF model can predict bulk free energy difference of peptides.,
FF,SinglePropertyPrediction,biobench_right_handed_population,This is a benchmark to evaluate how accurately an FF model can predict bulk free energy difference of peptides.,
FF,SinglePropertyPrediction,lj_2d_liquid_viscosity,This is a benchmark to evaluate how accurately an FF model can predict viscosity of Lennard-Jones liquid.,
-QC,EigenSolver,dft_3d_electron_bands_JVASP_816_Al_WTBH,This is a benchmark to evaluate how accurately an QC model can predict electronic bands of aluminum (JVASP-816) produced using Wannier tight binding Hamiltonian approach.,
+QC,EigenSolver,dft_3d_electron_bands_JVASP_816_Al_WTBH,This is a benchmark to evaluate how accurately an QC model can predict electronic bands of aluminum (JVASP-816) produced using Wannier tight binding Hamiltonian approach.,
\ No newline at end of file
diff --git a/jarvis_leaderboard/contributions/alignn_hydride_supercon/.DS_Store b/jarvis_leaderboard/contributions/alignn_hydride_supercon/.DS_Store
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diff --git a/jarvis_leaderboard/contributions/alignn_hydride_supercon/AI-SinglePropertyPrediction-Tc_supercon_hydride-dft_3d-test-mae.csv.zip b/jarvis_leaderboard/contributions/alignn_hydride_supercon/AI-SinglePropertyPrediction-Tc_supercon_hydride-dft_3d-test-mae.csv.zip
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diff --git a/jarvis_leaderboard/contributions/alignn_hydride_supercon/config.json b/jarvis_leaderboard/contributions/alignn_hydride_supercon/config.json
new file mode 100644
index 000000000..d1263b17c
--- /dev/null
+++ b/jarvis_leaderboard/contributions/alignn_hydride_supercon/config.json
@@ -0,0 +1,53 @@
+{
+ "version": "112bbedebdaecf59fb18e11c929080fb2f358246",
+ "dataset": "user_data",
+ "target": "target",
+ "atom_features": "cgcnn",
+ "neighbor_strategy": "k-nearest",
+ "id_tag": "jid",
+ "random_seed": 123,
+ "classification_threshold": null,
+ "n_val": null,
+ "n_test": null,
+ "n_train": null,
+ "train_ratio": 0.8,
+ "val_ratio": 0.1,
+ "test_ratio": 0.1,
+ "target_multiplication_factor": null,
+ "epochs": 300,
+ "batch_size": 16,
+ "weight_decay": 1e-05,
+ "learning_rate": 0.001,
+ "filename": "sample",
+ "warmup_steps": 2000,
+ "criterion": "mse",
+ "optimizer": "adamw",
+ "scheduler": "onecycle",
+ "pin_memory": false,
+ "save_dataloader": false,
+ "write_checkpoint": true,
+ "write_predictions": true,
+ "store_outputs": true,
+ "progress": true,
+ "log_tensorboard": false,
+ "standard_scalar_and_pca": false,
+ "use_canonize": true,
+ "num_workers": 0,
+ "cutoff": 8.0,
+ "max_neighbors": 12,
+ "keep_data_order": false,
+ "model": {
+ "name": "alignn",
+ "alignn_layers": 4,
+ "gcn_layers": 4,
+ "atom_input_features": 92,
+ "edge_input_features": 80,
+ "triplet_input_features": 40,
+ "embedding_features": 64,
+ "hidden_features": 256,
+ "output_features": 1,
+ "link": "identity",
+ "zero_inflated": false,
+ "classification": false
+ }
+}
diff --git a/jarvis_leaderboard/contributions/alignn_hydride_supercon/metadata.json b/jarvis_leaderboard/contributions/alignn_hydride_supercon/metadata.json
new file mode 100644
index 000000000..7cc8501fd
--- /dev/null
+++ b/jarvis_leaderboard/contributions/alignn_hydride_supercon/metadata.json
@@ -0,0 +1,17 @@
+{
+ "model_name": "ALIGNN",
+ "project_url": "https://iopscience.iop.org/article/10.1088/2752-5724/ad4a94",
+ "date_submitted": "05-16-2024",
+ "author_email": "daniel.wines@nist.gov",
+ "team_name": "ALIGNN",
+ "time_taken_seconds": {
+ "AI-SinglePropertyPrediction-Tc_supercon_hydride-dft_3d-test-mae.csv.zip": "15327"
+ },
+ "language": "python",
+ "os": "linux",
+ "software_used": "jarvis-tools,numpy,scipy,torch,alignn",
+ "hardware_used": "nisaba-cluster at NIST, V100 Tesla GPU",
+ "git_url": [
+ "https://github.com/usnistgov/alignn"
+ ]
+}
\ No newline at end of file
diff --git a/jarvis_leaderboard/contributions/alignn_hydride_supercon/run.sh b/jarvis_leaderboard/contributions/alignn_hydride_supercon/run.sh
new file mode 100644
index 000000000..472b06c9e
--- /dev/null
+++ b/jarvis_leaderboard/contributions/alignn_hydride_supercon/run.sh
@@ -0,0 +1,11 @@
+#!/bin/bash
+#SBATCH --nodes=1
+#SBATCH --ntasks-per-node=16
+#SBATCH --time=100:00:00
+#SBATCH --partition=mml
+#SBATCH --error=job3.err
+#SBATCH --output=job3.out
+
+
+conda activate alignn
+train_folder.py --root_dir "data/" --config "config.json" --output_dir=temp-3
diff --git a/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/.DS_Store b/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/.DS_Store
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diff --git a/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/AI-SinglePropertyPrediction-Tc_supercon_hydride_plus_bulk-dft_3d-test-mae.csv.zip b/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/AI-SinglePropertyPrediction-Tc_supercon_hydride_plus_bulk-dft_3d-test-mae.csv.zip
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diff --git a/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/config.json b/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/config.json
new file mode 100644
index 000000000..d1263b17c
--- /dev/null
+++ b/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/config.json
@@ -0,0 +1,53 @@
+{
+ "version": "112bbedebdaecf59fb18e11c929080fb2f358246",
+ "dataset": "user_data",
+ "target": "target",
+ "atom_features": "cgcnn",
+ "neighbor_strategy": "k-nearest",
+ "id_tag": "jid",
+ "random_seed": 123,
+ "classification_threshold": null,
+ "n_val": null,
+ "n_test": null,
+ "n_train": null,
+ "train_ratio": 0.8,
+ "val_ratio": 0.1,
+ "test_ratio": 0.1,
+ "target_multiplication_factor": null,
+ "epochs": 300,
+ "batch_size": 16,
+ "weight_decay": 1e-05,
+ "learning_rate": 0.001,
+ "filename": "sample",
+ "warmup_steps": 2000,
+ "criterion": "mse",
+ "optimizer": "adamw",
+ "scheduler": "onecycle",
+ "pin_memory": false,
+ "save_dataloader": false,
+ "write_checkpoint": true,
+ "write_predictions": true,
+ "store_outputs": true,
+ "progress": true,
+ "log_tensorboard": false,
+ "standard_scalar_and_pca": false,
+ "use_canonize": true,
+ "num_workers": 0,
+ "cutoff": 8.0,
+ "max_neighbors": 12,
+ "keep_data_order": false,
+ "model": {
+ "name": "alignn",
+ "alignn_layers": 4,
+ "gcn_layers": 4,
+ "atom_input_features": 92,
+ "edge_input_features": 80,
+ "triplet_input_features": 40,
+ "embedding_features": 64,
+ "hidden_features": 256,
+ "output_features": 1,
+ "link": "identity",
+ "zero_inflated": false,
+ "classification": false
+ }
+}
diff --git a/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/metadata.json b/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/metadata.json
new file mode 100644
index 000000000..c78fd04e1
--- /dev/null
+++ b/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/metadata.json
@@ -0,0 +1,17 @@
+{
+ "model_name": "ALIGNN",
+ "project_url": "https://iopscience.iop.org/article/10.1088/2752-5724/ad4a94",
+ "date_submitted": "05-16-2024",
+ "author_email": "daniel.wines@nist.gov",
+ "team_name": "ALIGNN",
+ "time_taken_seconds": {
+ "AI-SinglePropertyPrediction-Tc_supercon_hydride_plus_bulk-dft_3d-test-mae.csv.zip": "24672"
+ },
+ "language": "python",
+ "os": "linux",
+ "software_used": "jarvis-tools,numpy,scipy,torch,alignn",
+ "hardware_used": "nisaba-cluster at NIST, V100 Tesla GPU",
+ "git_url": [
+ "https://github.com/usnistgov/alignn"
+ ]
+}
\ No newline at end of file
diff --git a/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/run.sh b/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/run.sh
new file mode 100644
index 000000000..392396cbb
--- /dev/null
+++ b/jarvis_leaderboard/contributions/alignn_hydride_supercon_plusbulk/run.sh
@@ -0,0 +1,11 @@
+#!/bin/bash
+#SBATCH --nodes=1
+#SBATCH --ntasks-per-node=16
+#SBATCH --time=100:00:00
+#SBATCH --partition=mml
+#SBATCH --error=jobfull.err
+#SBATCH --output=jobfull.out
+
+
+conda activate alignn
+train_folder.py --root_dir "data/" --config "config.json" --output_dir=temp-full