Zobrazeno 1 - 3
of 3
pro vyhledávání: '"Janmey Jay Panda"'
Autor:
Krishna Rani Sahoo, Janmey Jay Panda, Sumit Bawari, Rahul Sharma, Dipak Maity, Ashique Lal, Raul Arenal, G. Rajalaksmi, Tharangattu N. Narayanan
Publikováno v:
Digital.CSIC. Repositorio Institucional del CSIC
Consejo Superior de Investigaciones Científicas (CSIC)
Consejo Superior de Investigaciones Científicas (CSIC)
Achieving room-temperature valley polarization in two-dimensional (2D) atomic layers (2D materials) by substitutional doping opens new avenues of applications. Here, monolayer MoS2, when doped with vanadium at low (0.1 atomic %) concentrations, is sh
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_dedup___::f507564104b8e3b0a0c3779ceeb568ff
http://hdl.handle.net/10261/280253
http://hdl.handle.net/10261/280253
Autor:
Satyaki Sasmal, Archit Bhardwaj, Janmey Jay Panda, Karthik V. Raman, Suman Mundlia, Saurabh Chaudhary, Lakshman Peri
Publikováno v:
Physical Review Applied. 14
Exchange-bias effect is a widely investigated topic for spintronic applications in magnetic data storage read heads and spin-valve sensors. This effect is observed in bilayers of magnetic materials comprising of a soft ferromagnet (FM) and an antifer
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::f1f2367f93d55a8e0985031948d77022
https://doi.org/10.1103/physrevapplied.14.024095
https://doi.org/10.1103/physrevapplied.14.024095
Autor:
Karthik V. Raman, Suman Mundlia, Janmey Jay Panda, Saurabh Chaudhary, Aathif Ahmedof, S. Mathimalar
Publikováno v:
Review of Scientific Instruments. 92:023906
Imaging atomically resolved surfaces and performing spectroscopy of exotic surfaces at cryogenic temperature in the presence of the magnetic field is an engineering challenge. Additionally, performing these measurements in an all-cryogen-free environ
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_dedup___::9efe39353fd6be5a19d4f0f10498da99
https://doi.org/10.1063/5.0041037
https://doi.org/10.1063/5.0041037