z-logo
Premium
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.

This content is not available in your region!

Continue researching here.

Having issues? You can contact us here
Accelerating Research

Address

John Eccles House
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom