Evaluation of the device characteristics of Bi2Sr2CaCu2O8+<i>δ</i> terahertz-wave emitters using wet-etching techniques

R R. Kikuchi (Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,) S S. Nakagawa (Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,) Y Y. Enomoto (Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,) Y Y. Kuzumi (Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,) S S. Yamada (Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,) K K. Maeshima Y Y. Yamauchi (Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,) H H. Minami (Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,) T T. Kashiwagi (Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,)

Abstract

Understanding the device characteristics associated with the shape and size of crystal chips is a key requirement for developing high-performance terahertz (THz) wave-emitting devices made of high-temperature superconductor Bi2Sr2CaCu2O8+δ(Bi2212) crystal chips, because these parameters reflect the emission frequency, emission power, self-heating conditions, and impedance matching. Wet-etching techniques are beneficial for creating comparable emitting chips from the same crystal fragment to further understand the above points regarding using Bi2212-crystal chips. Using wet-etching techniques, we prepared rectangular crystal chips with the same area using three different width (w) and length (L) aspect ratios and compared their emission characteristics. The range of the observed emission frequencies tended to be less dependent on the w/L ratio. However, the three samples differed significantly in terms of the excitation modes expected from the w/L ratio. When the aspect ratio approached one, the results indicated a tendency to resonate in the higher excitation modes. The excitation modes along the width of the chip were suppressed by decreasing the w/L ratio owing to the increased resonance frequencies of the transverse magnetic TM(m,0) modes. Although further studies are required, especially in terms of output enhancement, the results obtained herein are expected to aid in producing devices that can operate in the desired excitation mode.

Article Details

Volume / Issue Vol. 137, Issue 4
Published January 28, 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 (9)

R

R. Kikuchi

Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,

S

S. Nakagawa

Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,

Y

Y. Enomoto

Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,

Y

Y. Kuzumi

Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,

S

S. Yamada

Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,

K

K. Maeshima

Y

Y. Yamauchi

Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,

H

H. Minami

Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,

T

T. Kashiwagi

Graduate School of Pure & Applied Sciences, University of Tsukuba 1 , 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573,