TY - JOUR
T1 - Relaxation dynamics of optically excited quasi-particles in BSCCO
AU - Murakami, H.
AU - Yasuda, T.
AU - Tominari, Y.
AU - Kiwa, T.
AU - Tonouchi, M.
AU - Uchiyama, T.
AU - Iguchi, I.
AU - Wang, Z.
N1 - Funding Information:
This work was supported in part by a Grant-in-Aid for Scientific Research (B), nos. 12450146 and 13555107, from the Ministry of Education, Culture, Sports, Science and Technology. One of the authors (H.M.) wishes to acknowledge the support of the Murata Science Foundation.
PY - 2002/10/1
Y1 - 2002/10/1
N2 - To investigate the multi-excitation processes on the low-lying electronic structure of high-TC superconductors, time-domain pump and probe measurement has been carried out on under- and over-doped Bi2Sr2CaCu2O8+δ films. In the underdoped film, we found evidence for coexistence of two excitation states due to superconducting gap Δs and pseudogap Δp below TC. The observed relaxation processes of optically excited quasi-particles were well explained by two relaxation times of T-dependent τs and almost T-independent τp (0.7 ± 0.3 ps below 150 K). The τp existed up to T* ∼ 200 K and disappeared above 225 K. On the other hand, only one relaxation time, τs, was observed in the overdoped film at T = 10 K. The relaxation time, τs=4.2 ± 0.3 ps (below 40 K), for the underdoped sample was shorter than τs = 5.9 ± 0.2 ps (at T = 10 K) for the overdoped one, and about two times longer than τs = 2.1 ± 0.1 ps for YBa2Cu3O7-δ thin film.
AB - To investigate the multi-excitation processes on the low-lying electronic structure of high-TC superconductors, time-domain pump and probe measurement has been carried out on under- and over-doped Bi2Sr2CaCu2O8+δ films. In the underdoped film, we found evidence for coexistence of two excitation states due to superconducting gap Δs and pseudogap Δp below TC. The observed relaxation processes of optically excited quasi-particles were well explained by two relaxation times of T-dependent τs and almost T-independent τp (0.7 ± 0.3 ps below 150 K). The τp existed up to T* ∼ 200 K and disappeared above 225 K. On the other hand, only one relaxation time, τs, was observed in the overdoped film at T = 10 K. The relaxation time, τs=4.2 ± 0.3 ps (below 40 K), for the underdoped sample was shorter than τs = 5.9 ± 0.2 ps (at T = 10 K) for the overdoped one, and about two times longer than τs = 2.1 ± 0.1 ps for YBa2Cu3O7-δ thin film.
KW - BSCCO
KW - Pseudogap
KW - Relaxation time
KW - Thin film
KW - YBCO
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U2 - 10.1016/S0921-4534(02)01435-1
DO - 10.1016/S0921-4534(02)01435-1
M3 - Article
AN - SCOPUS:17144436275
SN - 0921-4534
VL - 378-381
SP - 320
EP - 323
JO - Physica C: Superconductivity and its applications
JF - Physica C: Superconductivity and its applications
IS - PART 1
ER -