“…The intensity is therefore determined by the Bose population of the magnons. Closer inspection of the 631 nm absorption region between 0.8 K and 4.2 K revealed a deviation from the T2 intensity law expected for a square planar Heisenberg ferromag with small anisotropy, because in this temperature range the thermal energy becomes comparable with the anisotropy gap in the magnon dispersion at the Brillouin zone centre (Day et al 1979). Furthermore, when the temperature is low enough to remove most of the intensity from the magnon-annihilation sideband ('h o t' band), a weak magnon-creation sideband ('cold' band) becomes apparent.…”
Section: Introductionmentioning
confidence: 91%
“…Rb2CrCl4 is a rare example of an ionic insulator which orders as a ferromagnet (Tc = 52.4 K) (see Day 1979 for a review). It is also unusual in having well-defined absorption bands in the visible, whose intensity is strongly reduced with the onset of magnetic order.…”
Section: Introductionmentioning
confidence: 99%
“…This structure is related to that of K 2NiF4 {DU space group) with a doubling of the unit cell in orthorhombic symmetry. This occurs because the high spin 3d4 configuration of Cr2+ has a ground state 5Eg in an octahedral field, two neighbouring units having their elongated, approximately tetragonal, axis along the directions [100] and [010] of K 2NiF4 (Day et al 1979 ;Munninghoff et al 1980 ;Janke et al 1983). The ground state suffers a zero-field splitting because of second-order mixing with excited states due to spin-orbit coupling.…”
Section: Introductionmentioning
confidence: 99%
“…The result of the competition between the ferromagnetic exchange and the anisotropy terms is a structure with spins on neighbouring ions canted at an angle + 6 from the easy [110] direction (Janke et al 1983) and the occurrence of a small gap in the acoustic spin-wave branch. Applying a magnetic field along one of the relatively hard [100] or hard [001] axes, this gap should first decrease to zero at a critical field B& or Bc and then rise again (Elliott et al 1980; Harrop The unusual temperature dependence of the visible absorption bands in Rb2CrCl4 has been the subject of several experimental studies (Day 1979 ;Janke et al 1982). Attention has concentrated on two regions, near 631 an 530 nm.…”
Eigenvalues and eigenfunctions of the spin waves in Rb
2
CrCl
4
, in the absence or presence of a magnetic field oriented along (or slightly off) one of the major crystallographic axes, are given in detail for the first time. We present a simple model to simulate the profiles of exchange induced exciton-magnon combination bands in canted ferromagnets, under various experimental conditions of temperature and magnetic field. This model is used to analyse new high-resolution magneto-optical data at low and very low (0.35 K) temperatures and to derive precise anisotropy parameters. It can be applied with only slight modifications to metamagnets showing axial or planar anisotropy.
“…The intensity is therefore determined by the Bose population of the magnons. Closer inspection of the 631 nm absorption region between 0.8 K and 4.2 K revealed a deviation from the T2 intensity law expected for a square planar Heisenberg ferromag with small anisotropy, because in this temperature range the thermal energy becomes comparable with the anisotropy gap in the magnon dispersion at the Brillouin zone centre (Day et al 1979). Furthermore, when the temperature is low enough to remove most of the intensity from the magnon-annihilation sideband ('h o t' band), a weak magnon-creation sideband ('cold' band) becomes apparent.…”
Section: Introductionmentioning
confidence: 91%
“…Rb2CrCl4 is a rare example of an ionic insulator which orders as a ferromagnet (Tc = 52.4 K) (see Day 1979 for a review). It is also unusual in having well-defined absorption bands in the visible, whose intensity is strongly reduced with the onset of magnetic order.…”
Section: Introductionmentioning
confidence: 99%
“…This structure is related to that of K 2NiF4 {DU space group) with a doubling of the unit cell in orthorhombic symmetry. This occurs because the high spin 3d4 configuration of Cr2+ has a ground state 5Eg in an octahedral field, two neighbouring units having their elongated, approximately tetragonal, axis along the directions [100] and [010] of K 2NiF4 (Day et al 1979 ;Munninghoff et al 1980 ;Janke et al 1983). The ground state suffers a zero-field splitting because of second-order mixing with excited states due to spin-orbit coupling.…”
Section: Introductionmentioning
confidence: 99%
“…The result of the competition between the ferromagnetic exchange and the anisotropy terms is a structure with spins on neighbouring ions canted at an angle + 6 from the easy [110] direction (Janke et al 1983) and the occurrence of a small gap in the acoustic spin-wave branch. Applying a magnetic field along one of the relatively hard [100] or hard [001] axes, this gap should first decrease to zero at a critical field B& or Bc and then rise again (Elliott et al 1980; Harrop The unusual temperature dependence of the visible absorption bands in Rb2CrCl4 has been the subject of several experimental studies (Day 1979 ;Janke et al 1982). Attention has concentrated on two regions, near 631 an 530 nm.…”
Eigenvalues and eigenfunctions of the spin waves in Rb
2
CrCl
4
, in the absence or presence of a magnetic field oriented along (or slightly off) one of the major crystallographic axes, are given in detail for the first time. We present a simple model to simulate the profiles of exchange induced exciton-magnon combination bands in canted ferromagnets, under various experimental conditions of temperature and magnetic field. This model is used to analyse new high-resolution magneto-optical data at low and very low (0.35 K) temperatures and to derive precise anisotropy parameters. It can be applied with only slight modifications to metamagnets showing axial or planar anisotropy.
“…(12) and (13) have been used for Rb 2 CrCl 4 and related systems in, e.g. [64][65][66][67][68][69][70][71]. Below only a few selected examples are explicitly provided.…”
The behaviour of the optical absorption bands of NaMnC1, is experimentally studied in the region of the 6Alg -f 4Alg, 4En(4G) transition of the Mn2+ ion in the temperature range 1.8 to 20 K and in magnetic fields up to 20 T. Exciton and its "hot" magnon sidebands are observed in the spectrum. The anomalous temperature dependence of the exciton-magnon bands intensity is explained by participation of magnons with wave vector k + 0 in absorption. The low energy exciton-magnon band is supposed to be due to simultaneous creation of an exciton and annihilation of three thermally created magnons. nonoc. nornoueHnfi NaMnC1, B Q~J I~C T M nepexoaa 6Alg + 4Alg, 4Eg(4G) HoHa Mnz+ B Coo6wam~ca pe3yJIbTaTbI 3KCnepMMeHTaJIbHOrO MCCJIeAOBaHElR IIOBeHeHHR OIITMYeCKMX TeMIlepaTypHOM MHTepBaJIe 1,8 A 0 20 K M B MarHHTHbIX ITOJIRX HO 20 T. B cneKTpe Ha-Gnronanacb 3KCMTOHHaR nOjIOCa M e6 "rOPRYMe" 3KCMTOH-MaI'HOHHbIe CIIYTHMKH. AHO-MaJIbHaFI TeMIIepaTypHaR 3aBMCHMOCTb HHTeHCMBHOCTM 3KCMTQH-MarHOHHbIX nOjlOC 065FICHReTCR YYaCTHeM B IIOrJIOweHHH MarHOHOB C BOJIHOBbIM BeKTOPOM k 0 . ripen-BpeMeHHblM POlKaeHkIeM 3KCklTOHa M YHHYTOl KeHMeM TpeX TepMHYeCKM B036YlfEHeHHbIX MWHOHOB.
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