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The [Fe(etz) 6 ](BF 4 ) 2 Spin‐Crossover System—Part One: High‐Spin ⇌ Low‐Spin Transition in Two Lattice Sites
Author(s) -
Hauser Andreas,
Gütlich Philipp,
Hinek Roland,
Spiering Hartmut,
Schollmeyer Dieter
Publication year - 1996
Publication title -
chemistry – a european journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.687
H-Index - 242
eISSN - 1521-3765
pISSN - 0947-6539
DOI - 10.1002/chem.19960021115
Subject(s) - spin crossover , spin transition , metastability , crystallography , population , condensed matter physics , chemistry , spin states , physics , demography , organic chemistry , sociology
The [Fe(etz),](BF,), spin‐cross‐over system (etz = 1‐ethyl‐1 H ‐tetrazole) crystallizes in space group P 1 , with the following lattice constants at 298 K: a 10.419(3), b=15.709(1), c = 18.890(2) Å = α = 71.223(9), β =77.986(10), and γ = 84.62(1)° V = 2862.0(9) Å 3 and Z = 3. Two nonequivalent lattice sites, one without (site A) and one with (site B) inversion symmetry, are observed. The population of the two sites n A : n B is 2:l. Iron(II) on site A undergoes a thermal low‐spin (LS) → high‐spin (HS) transition with T 1/2 I, = 105 K. whereas that on site B remains in the high‐spin state down to cryogenic temperatures. Application of external pressure of up to 1200 bar between 200 and 60 K does not cause formation of the low‐spin state on site B. On site A the high‐spin state can be populated as a metastable state at 20 K by irradiating the sample with λ = 514.5 nm; on site B a light‐induced population of the low‐spin state can be achieved with λ = 820 nm.