Picosecond evolution of an induced metallic state under infinitesimal optical doping in NdNiO3

B Basabendra Roy (Indian Institute of Science Education and Research Kolkata 1 , Mohanpur, Nadia 741246, West Bengal,) S Satyaki Kundu (Indian Institute of Science Education and Research Kolkata 1 , Mohanpur, Nadia 741246, West Bengal,) G Gaurav Dubey (Department of Physics, Indian Institute of Science Education and Research Bhopal 2 , Bhopal 462066,) P Priya Mahadevan (3 Department of Condensed Matter and Materials Physics, S.N. Bose National Center for Basic Sciences, JD-Block, Sector III, Salt Lake, Kolkata 700098, India) B Bipul Pal (Indian Institute of Science Education and Research Kolkata 1 , Mohanpur, Nadia 741246, West Bengal,) A Anamitra Mukherjee (School of Physical Sciences, National Institute of Science Education and Research, A CI of Homi Bhabha National Institute 4 , Jatni 752050,) D Dhanvir Singh Rana (Department of Physics, Indian Institute of Science Education and Research Bhopal 2 , Bhopal 462066,) B Bhavtosh Bansal (Indian Institute of Science Education and Research Kolkata 1 , Mohanpur, Nadia 741246, West Bengal,)

Abstract

NdNiO3 is a rare-earth nickelate where competing interactions yield a thermally induced metal–insulator transition accompanied by simultaneous structural and magnetic transitions. In recent years, femtosecond time resolved measurements have emerged as powerful tools for studying nonequilibrium phases in such complex systems. In this work, we demonstrate that even at 110 K, well below the insulator–metal transition temperature, an infinitesimal ≈0.1% optical doping in nickel’s d-band can destabilize the insulating phase into a long-lived metallic phase that builds up in the first 5 ps after the pulsed excitation. Using the hysteresis free nature of the first-order transition in our sample, we infer the true lattice temperature from resistance measurement. The threshold temperature for the runaway metallization is identified with the start of the phase coexistence region. We thus conclude that simultaneous electron–hole injection is at least an order of magnitude more effective in suppressing the transition than doping by electrons or holes alone. The results also demonstrate that the homeostasis-like situations responsible for the stability in such complex systems are nevertheless susceptible to catastrophic failures under certain types of infinitesimal perturbations.

Article Details

Volume / Issue Vol. 138, Issue 6
Published August 14, 2025
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (8)

B

Basabendra Roy

Indian Institute of Science Education and Research Kolkata 1 , Mohanpur, Nadia 741246, West Bengal,

S

Satyaki Kundu

Indian Institute of Science Education and Research Kolkata 1 , Mohanpur, Nadia 741246, West Bengal,

G

Gaurav Dubey

Department of Physics, Indian Institute of Science Education and Research Bhopal 2 , Bhopal 462066,

P

Priya Mahadevan

3 Department of Condensed Matter and Materials Physics, S.N. Bose National Center for Basic Sciences, JD-Block, Sector III, Salt Lake, Kolkata 700098, India

B

Bipul Pal

Indian Institute of Science Education and Research Kolkata 1 , Mohanpur, Nadia 741246, West Bengal,

A

Anamitra Mukherjee

School of Physical Sciences, National Institute of Science Education and Research, A CI of Homi Bhabha National Institute 4 , Jatni 752050,

D

Dhanvir Singh Rana

Department of Physics, Indian Institute of Science Education and Research Bhopal 2 , Bhopal 462066,

B

Bhavtosh Bansal

Indian Institute of Science Education and Research Kolkata 1 , Mohanpur, Nadia 741246, West Bengal,