Author:
Forslund Ola Kenji,Andreica Daniel,Sassa Yasmine,Imai Masaki,Michioka Chishiro,Yoshimura Kazuyoshi,Guguchia Zurab,Shermadini Zurab,Khasanov Rustem,Sugiyama Jun,Månsson Martin
Abstract
AbstractThe magnetic phase diagram of Sr$$_{1-x}$$
1
-
x
Ca$$_x$$
x
Co$$_2$$
2
P$$_2$$
2
as a function of hydrostatic pressure and temperature is investigated by means of high pressure muon spin rotation, relaxation and resonance ($$\mu ^+$$
μ
+
SR). The weak pressure dependence for the $$x\ne 1$$
x
≠
1
compounds suggests that the rich phase diagram of Sr$$_{1-x}$$
1
-
x
Ca$$_x$$
x
Co$$_2$$
2
P$$_2$$
2
as a function of x at ambient pressure may not solely be attributed to chemical pressure effects. The $$x=1$$
x
=
1
compound on the other hand reveals a high pressure dependence, where the long range magnetic order is fully suppressed at $$p_{\rm{c2}}\approx 9.8$$
p
c
2
≈
9.8
kbar, which seem to be a first order transition. In addition, an intermediate phase consisting of magnetic domains is formed above $$p_{\rm{c1}}\approx 8$$
p
c
1
≈
8
kbar where they co-exist with a magnetically disordered state. These domains are likely to be ferromagnetic islands (FMI) and consist of an high- (FMI-$$\textcircled {1}$$
1
) and low-temperature (FMI-$$\textcircled {2}$$
2
) region, respectively, separated by a phase boundary at $$T_{\rm{i}}\approx 20$$
T
i
≈
20
K. This kind of co-existence is unusual and is originating from a coupling between lattice and magnetic degrees of freedoms.
Funder
Royal Institute of Technology
Publisher
Springer Science and Business Media LLC
Cited by
1 articles.
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