
Himanshu Chakraborty
I am a member of Early Career Investigator Committee for Energy Frontier Research Center, and a postdoctoral fellow at the Institute of Computational Molecular Science, Temple University, US. Working towards the computational design of functional layered materials such as graphene nanostructures, layered metal-dichalcogenides, layered Borocarbonitrides, bulk and thin films of charge-transfer complexes etc.My research interests include computational material science, electronic structure calculations of such layered materials.Also, I am actively collaborating with various experimental and theoretical research groups around the world in the field of generation of clean fuel technology, e.g. understanding catalysis on the layered and two-dimensional materials such as borocarbonitrides , MoS2 etc. for hydrogen gas production
Supervisors: Prof. Michael L .Klein, Prof. C.N.R. Rao, Prof. Umesh V. Waghmare, and Prof. Alok Shukla
Phone: +1-484-274-0212
Address: 1925 N 12th St. SERC 701 E,
Temple University
Philadelphia, PA 19122
Supervisors: Prof. Michael L .Klein, Prof. C.N.R. Rao, Prof. Umesh V. Waghmare, and Prof. Alok Shukla
Phone: +1-484-274-0212
Address: 1925 N 12th St. SERC 701 E,
Temple University
Philadelphia, PA 19122
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Papers by Himanshu Chakraborty
tance for the development of next-generation, flexible, and fully
integrated energy, sensing, and artificial-intelligence technolo-
gies. Due to their exceptionally long spin lifetimes and strong
spin–charge interactions, these carbon materials could also
impact data transmission, processing, and storage. However, to
exploit these opportunities, the ability to directly convert energy
from spin information to electric charge is essential. Here,
we introduce a novel molecular spin–charge converter that is
comprised of a centimeter-sized free-standing organic charge-
transfer crystal. Magnetic-field effects in this material induce
intersystem crossings and spin–charge-lattice couplings that
generate an electric voltage for magnetic-energy harvesting.
The effective conversion between charge and spin stimulus
permits simultaneous and instantaneous self-powering and
sensing performance in a molecular crystal that displays ani-
sotropic behavior dependent on crystal orientation. We con-
firm the strong charge-transfer character of the crystals with
first principle calculations of the electronic density of states.
The solution processed flexible devices also exhibit an excellent
temperature sensitivity of <0.01 K and a unique piezoresistance
coefficient of −5.1 × 10 −6 Pa −1 . The self-powered sensing perfor-
mance of this molecular spin–charge converter, together with
its solution processability and flexibility, endow this molecular
charge-transfer crystal with the capability to drive a new gen-
eration of noncontact magnetic-energy harvesting and sensing
technologies.
computations have been performed using the pi-electron Pariser-Parr-Pople model Hamiltonian, which incorporates long-range Coulomb interactions. The influence of electron correlation effects on the ground and excited states has been included by means of the configuration-interaction approach, used at various levels. Our calculations have revealed that the absorption spectra are red-shifted with the increasing sizes of quantum dots. It has been observed that the first peak of the linear optical absorption, which represents the optical gap, is not the most intense peak. This result is in excellent agreement with the experimental data, but in stark contrast to the predictions of the tight-binding model, according to which the first peak is the most intense peak, pointing to the importance of electron-correlation effects. Furthermore, an analysis of the wave functions of the excited states contributing to the spectra reveals the presence of plasmonic effects.
tance for the development of next-generation, flexible, and fully
integrated energy, sensing, and artificial-intelligence technolo-
gies. Due to their exceptionally long spin lifetimes and strong
spin–charge interactions, these carbon materials could also
impact data transmission, processing, and storage. However, to
exploit these opportunities, the ability to directly convert energy
from spin information to electric charge is essential. Here,
we introduce a novel molecular spin–charge converter that is
comprised of a centimeter-sized free-standing organic charge-
transfer crystal. Magnetic-field effects in this material induce
intersystem crossings and spin–charge-lattice couplings that
generate an electric voltage for magnetic-energy harvesting.
The effective conversion between charge and spin stimulus
permits simultaneous and instantaneous self-powering and
sensing performance in a molecular crystal that displays ani-
sotropic behavior dependent on crystal orientation. We con-
firm the strong charge-transfer character of the crystals with
first principle calculations of the electronic density of states.
The solution processed flexible devices also exhibit an excellent
temperature sensitivity of <0.01 K and a unique piezoresistance
coefficient of −5.1 × 10 −6 Pa −1 . The self-powered sensing perfor-
mance of this molecular spin–charge converter, together with
its solution processability and flexibility, endow this molecular
charge-transfer crystal with the capability to drive a new gen-
eration of noncontact magnetic-energy harvesting and sensing
technologies.
computations have been performed using the pi-electron Pariser-Parr-Pople model Hamiltonian, which incorporates long-range Coulomb interactions. The influence of electron correlation effects on the ground and excited states has been included by means of the configuration-interaction approach, used at various levels. Our calculations have revealed that the absorption spectra are red-shifted with the increasing sizes of quantum dots. It has been observed that the first peak of the linear optical absorption, which represents the optical gap, is not the most intense peak. This result is in excellent agreement with the experimental data, but in stark contrast to the predictions of the tight-binding model, according to which the first peak is the most intense peak, pointing to the importance of electron-correlation effects. Furthermore, an analysis of the wave functions of the excited states contributing to the spectra reveals the presence of plasmonic effects.