Date:
Thu, 29/05/202512:00-13:30
Location:
Danciger B seminar room
Lecturer: Amos Sharoni, Department of Physics, Bar Ilan University
Abstract:
The ramp reversal memory (RRM) is a non-volatile memory effect we discovered
originally in correlated oxides with temperature-driven insulator-metal transitions
(IMT), such as VO2, V2O3 and NdNiO3. The memory appears as a resistance increase at
predefined temperatures that are set or erased by simple heating-cooling (i.e., ramp-
reversal) protocols. The characteristics of this memory effect do not coincide with any
previously reported history or memory effects.
In this talk we will review our current understanding of the RRM. We will overview
the main properties of the memory effect, show how the memory appears in different
systems, discuss what features are system dependent, and review the ingredients
required for the effect to arise. We will conclude that the RRM is indeed an emergent
phenomenon, where the underlying physical mechanism can change from system to
system. Thus, it is expected to appear in additional materials with relevant ingredients.
[1] N. Vardi, E. Anouchi, T. Yamin, S. Middey, M. Kareev, J. Chakhalian, Y. Dubi, and A. Sharoni,
Ramp-Reversal Memory and Phase-Boundary Scarring in Transition Metal Oxides, Advanced
Materials 29, 1605029 (2017).
[2] E. Anouchi, N. Vardi, Y. Kalcheim, I. K. Schuller, and A. Sharoni, Universality and microstrain
origin of the ramp reversal memory effect, Phys. Rev. B 106, 205145 (2022).
[3] A. Fried, E. Anouchi, G. Cohen Taguri, J. Shvartzberg, and A. Sharoni, Film morphology and
substrate strain contributions to ramp reversal memory in VO2, Phys. Rev. Mater. 8, 015002
(2024).
[4] A. Fried, O. Gotesdyner, I. Feldman, A. Kanigel, and A. Sharoni, Ramp Reversal Memory in
Bulk Crystals of 1T-TaS2, arXiv:2409.11977 (2024).
Abstract:
The ramp reversal memory (RRM) is a non-volatile memory effect we discovered
originally in correlated oxides with temperature-driven insulator-metal transitions
(IMT), such as VO2, V2O3 and NdNiO3. The memory appears as a resistance increase at
predefined temperatures that are set or erased by simple heating-cooling (i.e., ramp-
reversal) protocols. The characteristics of this memory effect do not coincide with any
previously reported history or memory effects.
In this talk we will review our current understanding of the RRM. We will overview
the main properties of the memory effect, show how the memory appears in different
systems, discuss what features are system dependent, and review the ingredients
required for the effect to arise. We will conclude that the RRM is indeed an emergent
phenomenon, where the underlying physical mechanism can change from system to
system. Thus, it is expected to appear in additional materials with relevant ingredients.
[1] N. Vardi, E. Anouchi, T. Yamin, S. Middey, M. Kareev, J. Chakhalian, Y. Dubi, and A. Sharoni,
Ramp-Reversal Memory and Phase-Boundary Scarring in Transition Metal Oxides, Advanced
Materials 29, 1605029 (2017).
[2] E. Anouchi, N. Vardi, Y. Kalcheim, I. K. Schuller, and A. Sharoni, Universality and microstrain
origin of the ramp reversal memory effect, Phys. Rev. B 106, 205145 (2022).
[3] A. Fried, E. Anouchi, G. Cohen Taguri, J. Shvartzberg, and A. Sharoni, Film morphology and
substrate strain contributions to ramp reversal memory in VO2, Phys. Rev. Mater. 8, 015002
(2024).
[4] A. Fried, O. Gotesdyner, I. Feldman, A. Kanigel, and A. Sharoni, Ramp Reversal Memory in
Bulk Crystals of 1T-TaS2, arXiv:2409.11977 (2024).