Table 1 Mössbauer parameters extracted from the fitting of the spectra at T = 2.2 K and from ab initio calculations

From: Mössbauer spectroscopy of a monolayer of single molecule magnets

 

Parameter

Central site

Peripheral sitesf

Dropcast

Isomer shift (mm s−1)a

0.409 (2)

0.418 (4)

0.467 (2)

0.467 (2)

Electric quadrupole shift (mm s−1)b

−0.149 (2)

0.045 (4)

0.094 (2)

0.094 (2)

Hyperfine magnetic field (T)

46.39 (1)

52.72 (2)

52.92 (2)

52.92 (2)

Dropcast (theory)

 

Fe1

Fe2

Fe3

Fe4

Hyperfine magnetic field, Aiso (T)c

46.90

52.34

54.49

53.32

Monolayer

Isomer shift (mm s−1)a

0.27 (5)

0.43 (4)

0.42 (6)

0.42 (6)

Electric quadrupole shift (mm s−1)b

−0.07 (4)

−0.06 (2)

−0.03 (2)

−0.03 (2)

σ of Gaussian broadening (mm s−1)

0.28 (6)

0.25 (5)

0.2 (1)

0.2 (1)

Hyperfine magnetic field (T)

40.7 (4)

49.9 (3)

45.6 (9)

45.6 (9)

Monolayer (theory)

 

Fe1

Fe2

Fe3

Fe4

Hyperfine magnetic field, Aiso (T)c,d

43.68 (W1)

52.11 (W1)

52.22 (W1)

53.04 (W1)

45.09 (W3)

52.50 (W3)

51.73 (W3)

49.04 (W3)

 

ΔAiso (T) due to Au substratee

−1.77

−0.28

−0.55

−0.60

  1. aWith respect to α-Fe
  2. bThe formula of the electric quadrupole shift is \({\it{\epsilon }} = \frac{{e^2qQ}}{4}\left( {\frac{{3{\mathrm{cos}}^2\theta - 1}}{2}} \right)\), where θ is the angle between the electric field gradient principal axis and the direction of the hyperfine magnetic field at the iron atom
  3. cThe calculated hyperfine fields (Fermi contact terms) take into account the \(\left\langle {s_z^i} \right\rangle\) value and were scaled by a factor of 1.81 (see text and Methods section)
  4. dGeometries resulting from two different AIMD trajectories as in26, i.e., walker 1 (W1) and walker 3 (W3), were considered
  5. eReduction of Aiso (T) values due to pure electronic effects induced by the substrate. The ΔAiso values were calculated as 22Δ\(\left\langle {s_z^i} \right\rangle\) (averaged over all AIMD walkers) from the variation of the spin density, computed at the GPW-DFT level, between-on-surface and extrapolated geometries
  6. fThe numbering of peripheral sites only applies to computed values; experimental parameters in the last column apply to two indistinguishable sites, errors are given in parentheses