Research topics:

Development of terahertz, infrared, and optical metamaterial based active and passive plasmonic devices.

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Figure S6.rar
Feb 18, 2021 - Replication Data for: Strong Self-trapping by Deformation Potential Limits Photovoltaic Performance in Bismuth Double Perovskite
RAR Archive - 274.2 KB - MD5: c538b2012f752830d942194b3f5acbfc
Data
replicating data for Supplementary Figure S6
Figure S7.rar
Feb 18, 2021 - Replication Data for: Strong Self-trapping by Deformation Potential Limits Photovoltaic Performance in Bismuth Double Perovskite
RAR Archive - 306.3 KB - MD5: 646b48f848ee7ee334e2d80b2b9d4b3a
Data
replicating data for Supplementary Figure S7
Figure S8.rar
Feb 18, 2021 - Replication Data for: Strong Self-trapping by Deformation Potential Limits Photovoltaic Performance in Bismuth Double Perovskite
RAR Archive - 505.7 KB - MD5: ef27859688d2300c12bd6bbb039c24a0
Data
replicating data for Supplementary Figure S8
Figure S9.rar
Feb 18, 2021 - Replication Data for: Strong Self-trapping by Deformation Potential Limits Photovoltaic Performance in Bismuth Double Perovskite
RAR Archive - 2.5 MB - MD5: 6d383a41b4ebc3da55bad6382a3f7911
Data
replicating data for Supplementary Figure S9
Replication Data for: Impact of conductivity on Lorentzian and Fano resonant high-Q THz metamaterials: Superconductor, metal and perfect electric conductor
Replication Data for: Impact of conductivity on Lorentzian and Fano resonant high-Q THz metamaterials: Superconductor, metal and perfect electric conductor
May 15, 2020 - Yogesh Kumar Srivastava
Srivastava, Yogesh Kumar; Singh, Ranjan, 2020, "Replication Data for: Impact of conductivity on Lorentzian and Fano resonant high-Q THz metamaterials: Superconductor, metal and perfect electric conductor", https://doi.org/10.21979/N9/AWKV0V, DR-NTU (Data), V1
High temperature superconductors have created exciting opportunities for switchable metamaterial and plasmonic devices operating at terahertz frequencies. In recent times, there have been several demonstrations using superconducting metamaterials, such as thermal, electrical, mag...
Figure 2 a.opj
May 15, 2020 - Replication Data for: Impact of conductivity on Lorentzian and Fano resonant high-Q THz metamaterials: Superconductor, metal and perfect electric conductor
Unknown - 72.0 KB - MD5: 5873da31518249e0e53363fca7988550
Data
Figure 2 b.opj
May 15, 2020 - Replication Data for: Impact of conductivity on Lorentzian and Fano resonant high-Q THz metamaterials: Superconductor, metal and perfect electric conductor
Unknown - 68.4 KB - MD5: 4cbc8d5cca929f8be64fbb885b88b0dd
Data
Figure 2 c.opj
May 15, 2020 - Replication Data for: Impact of conductivity on Lorentzian and Fano resonant high-Q THz metamaterials: Superconductor, metal and perfect electric conductor
Unknown - 74.3 KB - MD5: 444924f9d246a313b5dc949df5e4dcc4
Data
Figure 2 d.opj
May 15, 2020 - Replication Data for: Impact of conductivity on Lorentzian and Fano resonant high-Q THz metamaterials: Superconductor, metal and perfect electric conductor
Unknown - 68.4 KB - MD5: 22811c1e0794ce8df5fc5a36cf1f205f
Data
Figure 3 a.opj
May 15, 2020 - Replication Data for: Impact of conductivity on Lorentzian and Fano resonant high-Q THz metamaterials: Superconductor, metal and perfect electric conductor
Unknown - 79.0 KB - MD5: 12cf24e907e7840dd726dc88e3e56a78
Data
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