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Reversible Control of Crystalline Rotors by Squeezing Their Hydrogen Bond Cloud Across a Halogen Bond-Mediated Phase Transition

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Supporting Information for

Reversible control of crystalline rotors by squeezing their hydrogen bond cloud across a halogen bond-mediated phase transition

Cyprien Lemouchi, Hiroshi M. Yamamoto, Reizo Kato, Sergey Simonov, Leokadiya Zorina, Antonio Rodríguez-Fortea, Enric Canadell, Pawel Wzietek, Konstantinos Iliopoulos, Denis Gindre, Michael Chrysos and Patrick Batail*

This file contains:

Figure S1. Temperature dependence of unit cell parameters for 2.

Figure S2. Relative orientation of an inner rotator and its surrounding phenyl platforms for 

= 0°.

Table S1. Crystallographic data.

Table S2. C–H···I–C (Å) and C–I···I–C (Å) interactions in 2.

Table S3. Calculated energies as a function of  for 2 at 90 K and 298 K

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Figure S1. Temperature dependence of unit cell parameters for 2. For clarity of the description of the relative changes, lattice parameters for the low-temperature phase are transformed to high-temperature triclinic unit cell. Doubling of the lattice at the transition temperature is not considered here.

6.9 6.92 6.94 6.96 6.98 7

80 110 140 170 200 230 260 290

a (Å)

T (K)

cooling heating

9.1 9.12 9.14 9.16

80 110 140 170 200 230 260 290

b (Å)

T (K)

cooling heating

83.2 83.4 83.6 83.8 84 84.2

80 110 140 170 200 230 260 290

γ angle (°)

T (K)

cooling heating

640 650 660

80 110 140 170 200 230 260 290

V3)

T (K)

cooling heating

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3

Table S1. Crystal data, data collection and refinement details for 2

Temperature / K 293 90

λ / Å 0.71073 0.71073

Chemical formula C24H12F6I4 C24H12F6I4

Molecular weight 921.94 921.94

Crystal system triclinic triclinic

a / Å 7.0104(3) 9.0986(5)

b / Å 9.1585(6) 11.2261(7)

c / Å 10.9366(6) 13.7829(6)

/ ° 80.332(6) 112.913(5)

β / º 73.993(4) 96.345(5)

 / ° 84.208(4) 93.942(5)

V / Å3 664.26(6) 1279.1(1)

Space group, Z P1, 1 P1, 2

F(000) 422 844

ρcalc. / g·cm-3 2.305 2.394

μ / cm-1 47.44 49.27

Tmin, Tmax 0.5422, 0.7460 0.5564, 0.7479

max / º 60.0 79.6

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Reflections collected 26080 75631

Independent reflections 3855 15628

Rint 0.0344 0.0296

No. of parameters 199 307

GooF on F2 1.085 1.075

R1 [I>2(I)] 0.0429 0.0262

wR2[I>2(I)] 0.1120 0.0491

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Table S2. C–H···I–C (Å) and C–I···I–C (Å) interactions in 2 and BIBCO3; the same, yet activated16 interactions in the radical cation salt, -(EDT-TTF-I2)2•+[(Pb5/6[lead

vacancy]1/6I2)1/3–]325 and Dehnicke-Weiss’s [PPh4+][ diiodoacetylene][I]26

2

Rotator-Stator Stator-Stator

C–H···I–C (Å) C–H···F–C (Å) C–I···I–C (Å)

293 K total rotor site

occupancies:

0.3 + 0.2 + 0.3 + 0.2

30% occupancy 3.304 3.343

30% occupancy 2.640

2.894 in-plane:

3.991 transverse:

4.041 20% occupancy

3.231 3.338 3.352

20% occupancy 2.520 2.655

90 K one single site

3.211 3.270 3.294 3.347

2.714 2.803 2.797

in-plane:

4.188 3.796 transverse:

3.901

BIBCO3

295 K 3.089

3.278 3.325

4.005 4.062

90 K

3.072 3.094 3.107 3.237 3.251 3.274 3.296 3.307 3.309 3.344

3.933 3.952 3.967 3.973 3.996 4.008

F F

I

F F

I F

I F

I

I I

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C–H···Br (Å)14f 3.2932(7)

-(EDT-TTF-I2)2•+[(Pb5/6(lead vacancy)1/6I2)1/3–]325

C–H···I–C (Å) 1

C–H···(I–Pb)anion (Å) 2

C–I···(I–Pb)anion (Å) 3

3.019 2.746 3.788

S S

I I S S S

S H

HH H

S S I

I S

S S

S H HH

H I I

I I I I

I I I I I I

1 2

3

1/2

1/2

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[PPh4+][ diiodoacetylene[I] 26 C–I···I (Å)

3.271 and 3.351

25 T. Devic, M. Evain, Y. Moelo, E. Canadell, P. Auban-Senzier, M. Fourmigué and P. Batail, J. Am. Chem. Soc. 2003, 125, 3295- 3301; T. Devic, E. Canadell, P. Auban-Senzier and P. Batail, J. Mater. Chem. 2004, 14, 135-137.

26 M. Ghassemzadeh, K. Harms, K. Dehnicke and D. Fenske, Z. Naturforsch. B 1994, 49, 593-601; M. Ghassemzadeh, J. Magull, D. Fenske and K. Dehnicke, Z. Naturforsh. B 1996, 51, 1579-1582; J. Grebe, G. Geiseler, K. Harms and K. Dehnicke, Z.

Naturforsh. B 1999, 54, 77-86.

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Table S3. Calculated energies (see Figure 7c) as a function of  for 2 at 90 K (left) and 298 K (right) when the six CH2 groups as well as the iodine atoms of the six fragments representing the environment are allowed to relax.

Figure S2. Relative orientation of an inner rotator and its surrounding phenyl platforms for 

= 0°.  is the dihedral angle that involves one C—C bond axle of a rotator blade and the normal to one vicinal phenyl ring, as shown by red dashed lines.

Structure 298 K

(deg) E (au) E rel (kcal/mol)

0 -115866.8032000 0.37

10 -115866.8035106 0.18

20 -115866.8027587 0.65

30 -115866.8027241 0.67

40 -115866.8028505 0.59

50 -115866.8033954 0.25

60 -115866.8037931 0.00

70 -115866.8031711 0.39

80 -115866.8025690 0.77

90 -115866.8027315 0.67

100 -115866.8030960 0.44

110 -115866.8032623 0.33

120 -115866.8034276 0.23

Structure 90 K

(deg) E (au) E rel (kcal/mol)

0 -115866.8219840 0.01

10 -115866.8211673 0.52

20 -115866.8196810 1.46

30 -115866.8178000 2.64

40 -115866.8177680 2.66

50 -115866.8176340 2.74

60 -115866.8188890 1.95

70 -115866.8188490 1.98

80 -115866.8181856 2.39

90 -115866.8184254 2.24

100 -115866.8200739 1.21

110 -115866.8216411 0.23

120 -115866.8219999 0.00

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