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Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

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Page 1: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Continuous Symmetry and Chirality Measures

David Avnir

Institute of ChemistryThe Hebrew University of Jerusalem

Harvard, Boston, January 28, 2013

Page 2: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 3: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 4: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 5: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 6: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 7: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

“Near” C2 symmetry: HIV Protease mutant V82A complexed with A77 inhibitor

What, quantitatively, is the C2 symmetry content of that protein?

Page 8: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Gradual changing chirality and C2-ness in aggregates

Is it possible to quantify these changes?

Page 9: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 10: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Since achirality relates to symmetry, similar questions pop up also in the context of chirality:

“By how much is one molecule more chiral than the other?”

Page 11: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

In fact, asymmetry and chirality are very common:

Given a sufficiently high resolution in space or time it is quite difficult to find a fully symmetric, achiral molecule.

Consider watching methane on a vibrational time-scale:

Only one in zillion frames will show the following:

Page 12: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Given a sufficiently high resolution in space or time it is quite difficult to find a fully symmetric, achiral molecule

Spatial resolutions:

Often, symmetry is lost at the condensed phase:

# An adsorbed molecule

# A matrix-entrapped molecule

# A molecule packed in the crystal

# A molecule in the glassy state

# A molecule within a cluster

Page 13: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

A methodology is needed in order to quantify the degree of symmetry and the degree of chirality:

#Comparing different molecules

#Following changes within a single molecule

Page 14: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The proposed methodology for a symmetry-measure design:

Find the minimal distance between the original structure, and the one obtained after the G point-group symmetry is operated on it.

Page 15: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The continuous symmetry measure

* The scale is 0 - 1 (0 - 100):

The larger S(G) is, the higher is the deviation from G-symmetry

N

1k

2

2ˆ1

min100 kk QQNd

)S(G

kQ

kQצ

: The original structure

: The symmetry-operated structure

N : Number of vertices

d : Size normalization factor

H. Zabrodsky

Page 16: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

E

C3

C32

Measuring the degree of C3-ness (S(C3)) of a triangle

Ch. Dryzun

Page 17: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

All three triangles are superimposed. The set of 9 points is C3-symmetric. Its blues average is a C3-symmetric triangle

The measure is the collection of distances between the blue and the (original) red

Page 18: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

G: The achiral symmetry point group which minimizes S(G)

Achiral molecule: S(G) = 0

The more chiral the molecule is, the higher is S(G)

S(G) as a continuous chirality measure

N

1k

2

2ˆ1

min100 kk QQNd

)S(G

Page 19: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The Continuous Shape Measure

S. Alvarez, P. Alemany

* The CSM estimates the distance to an a-priori unknown shape with the desired symmetry

* The Shape Measure estimates the minimal distance to a specific pre-selected shape (any shape)

* For ML6:

# Shape: What is the degree of ML6-

octahedricity (S(L6-Oh))?

# Symmetry: What is the degree of Oh-ness

(S(Oh))? D4h-ness (S(D4h)? And of S(D2h)?

Page 20: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

* The measure is a global structural parameter: It takes into account all bond angles and bond lengths

* A full profile of symmetry and chirality values is obtained

* All values are comparable either within the same molecule or between different ones

* The computational tools are efficient

* Analytical solutions have been obtained for many types of symmetry

* The shape of the nearest symmetric object is an outcome

* The measure is well behaved, and its correlations with physical/chemical parameters agree with intuition

Some properties of the symmetry measure

Page 21: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Planar square – D4h

The CSM values of an AB4 species

with respect to tetrahedricity and planar-squareness

Distorted tetrahedron

S(Td) = 0

S(D4h) = 33.3

S(Td) = 10.6

S(D4h) = 7.84

S(Td) = 33.3

S(D4h) = 0

Perfect tetrahedron - Td

Page 22: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

0 10072.22

Td

D4h

C3v

Cv

33.33 65.73

0 1

S(Td)

The full scale of the CSM

Page 23: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 24: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

S(TP)

[Ta(CCSitBu3)6]- [Ti2(-SMe)3(SMe)6]2-[Zr(SC6H4-4-OMe)6]2-

1.88

18.8°

1.67

8.27

5.51

1.34

33.3°

4.45

3.94

2.16

30.4°

5.09

S(chir)

S(Oh)

The most chiral monodentate complex

Page 25: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 26: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Trends within families and classifications

Symmetry maps

Page 27: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The symmetry map of 13,000 transition metal ML4 complexes

S. Alvarez, P. Alemany, JACS 2004

Page 28: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

0

5

10

15

20

25

30

0 5 10 15 20 25 30

CuCl42-: The tetrahedral to planar-square symmetry map and pathway

S(Td)

S(D

4h)

S. Keinan

Page 29: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Several possible pathways for this transformation

Spread

Twist

Compression

70o

110o

Page 30: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

0

5

10

15

20

25

30

0 5 10 15 20 25 30

The tetrahedral to planar-square transformation 

Spread

Twist

Compression

CuCl42-

S(Td)

S(D

4h)

Page 31: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

30

25

20

15

10

5

035302520151050

-2033.20-2033.15-2033.10-2033.05-2033.00-2032.95

d

JS(D

)

S(T )

-2033.15-2033.10

-2033.05

-2033.00

(136.8 kcal/mol)(105.4 kcal/mol)(74.1 kcal/mol)(42.67 kcal/mol)(11.29 kcal/mol)

J -2033.168 (0 Kcal/mol)

Spread simulation

Energy in Hartree (relative energy in kcal/mol)

Minimal energy and minimal symmetry values coincide

•S

( D4 h

)

Page 32: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Tetracoordinated Bis-Chelate Metal Complexes

M(L-L')2: The [M(bipy)2] family

L-M-L bond angles:

# Spread From 90° to 109.4°

#Two Twist pathways: The bidentate nature is introduced by keeping the two opposite L-M-L bond angles constant at typical 82 and 73°

70o

110o

Twist

Page 33: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

We (mainly S. Alvarez) analyzed similarly all MLn families with n from 4 to 10

4 Chem. Eur. J., 10, 190-207 (2004).

5 J. Chem. Soc., Dalton Trans., 3288-3303 (2000).

6 New J. Chem., 26, 996-1009 (2002).

7 Chem. Eur. J., 9, 1281-1295 (2003).

8 Chem. Eur. J., 11, 1479 (2005).

9 Inorg. Chem., 44, 6939-6948 (2005).

10 Work in progress

Page 34: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Symmetry or chirality as reaction coordinates

Page 35: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Stone-Wales Enantiomerizations in Fullerenes

Y. Pinto, P. Fowler (Exeter)

Page 36: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Hückel energy changes along the enantiomerization

Page 37: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The sensitivity of energy/chirality dependence on the size of the fullerene

Page 38: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Temperature and pressure effects

on symmetry and chirality

Page 39: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Cl

NH3+

150

200

250

300

0.34 0.35 0.36 0.37 0.38 0.39

Tem

p (o K

)

S(Oh)

Data: Wei, M. & Willett, R.D. Inorg. Chem. (1995) 34, 3780. Analysis: S. Keinan

Changes in the degree of octahedricity

with temperature

CuCl64-

Page 40: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Low QuartzSiO2, P3221

Temperature and pressure effects on the chirality and symmetry of extended materials:

Quartz

Page 41: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The building blocks of quartz

SiO4 Si(OSi)4

SiSi4-O(SiO3)4-

Page 42: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Combining temperature and pressure effects through symmetry analysis

b

0

0.5

1

1.5

2

2.5

3

3.5

4

120 130 140 150SiOSi angle

C2

A

B

C

D

T

S(C2) of a four tetrahedra unit:

A measure of helicity

A correlation between global and specific geometric parameters

Page 43: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

0 5 10 15

0

0.05

0.1

0.15

0.2

0.25

0.3

0.35

0.4

0.45

0 5 10 15Pressure (GPa)

Te

tra

he

dri

city

GeO4

SiO4

GeO4

SiO4

a

b

20 SiO2

GeO2

SiO2

GeO2

20

GeGe4

SiSi4

0 5 10 15

0

0.05

0.1

0.15

0.2

0.25

0.3

0.35

0.4

0.45

0 5 10 15Pressure (GPa)

Te

tra

he

dri

city

GeO4

SiO4

GeO4

SiO4

0

0.05

0.1

0.15

0.2

0.25

0.3

0.35

0.4

0.45

0 5 10 15Pressure (GPa)

Te

tra

he

dri

city

GeO4

SiO4

GeO4

SiO4

GeO4

SiO4

a

b

20 SiO2

GeO2

20 SiO2

GeO2

SiO2

GeO2

20 SiO2

GeO2

20 SiO2

GeO2

20 SiO2

GeO2

20

GeGe4

SiSi4

GeO

SiO

4

4

4

4

4

4

Predicting the high pressure symmetry behavior of quartz based on the isostrucutral GeO2

D. Yogev-Einot , D. Avnir; Acta Cryst. (2004) B60 163-173

Page 44: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The building blocks of quartz: All are chiral!

SiO4 Si(OSi)4

SiSi4-O(SiO3)4-

Page 45: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

M. Pinsky et al, “Statistical analysis of the estimation of distance measures” J. Comput. Chem., 24, 786–796 (2003)

How small can the measure be and still indicate chirality?

The error bar

# Typical limit: In quartz, S(Chir) of SiO4 = 0.0007

# For S values near zero, the error bar is not symmetric: The + and - are different.

# If the lower bound of S touches 0.00000, then the molecule is achiral.

Page 46: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

0.97

1.02

1.07

1.12

1.17

98 298 498 698 898 1098

Temperature (°K)

Le

Cha

teli

er

t

The optical rotation of quartz

Le Chatelier, H. Com. Rend de I'Acad Sciences 1889, 109, 264.

Page 47: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

0.97

1.02

1.07

1.12

1.17

98 298 498 698 898 1098

Temperature ( K)

0.54

0.56

0.58

0.6

0.62

0.64

Temperature (°K)

Le

Cha

teli

er

t

Ch

irality, SiSi4

Chirality t

115 years later: Interpretation and exact match with quantitative chirality changes

Crystallography: Kihara, 1990. Analysis: D. Yogev-Einot

SiSi4

Page 48: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Correlations between continuous symmetry and spectral properties

Page 49: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

7000

8000

9000

10000

11000

12000

13000

14000

15000

0 5 10 15 20 25 30 35S(Td)

max d-d

(c

m-1)

Jahn-Teller effects and symmetry:

The d-d splitting in Cu complexes

Data: Halvorson, 1990. Analysis: S. Keinan

Page 50: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Changes in transition probability as a function of octahedricity

CuN4O2 Chromophores:

S(Oh)

N

Cu NN

N

O2N

H

HH

H

(a)

(c) (b)

50

100

150

200

250

1 2 3 4 5 6 7

a=b=c=(CH2)3

a=b=c=(CH2)2

a=c=(CH2)3; b=(CH2)2

a=c=(CH2)2; b=(CH2)3

[c

m-1M

-1]

Data: P. Comba, 1999

+2H2O

Page 51: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Degree of allowedness of ESR transition

as a function of the degree of tetrahedricity

Page 52: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

z

x

y

z

x

y

Maximal and minimal shielding in AB4 species

Symmetry effects on NMR chemical shielding

Page 53: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Current wisdom:

But how does the shielding change when the symmetry changes continuously?

Page 54: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

350

0 10 20 30 40

0

50

100

150

200

250

300C

SA

(ppm

)

S(D4h) – deviation from planarity

CSA vs. S(D4h)200 randomly distorted SiH4

All 29Si NMR properties were calculated using Gaussian98, B3LYP/6-31G* and GIAO

A. Steinberg, M. Karni

Page 55: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

0

50

100

150

200

250

300

350

RandomSpread: Maximal de-shielding

0 10 20 30 40

S(D4h) – deviation from planarity

CSA

(ppm

)

CSA vs. S(D4h)

If you de le te a

parag raphmark, the

follow ing

Page 56: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Correlation between symmetry/chirality

and chemical recognition

* Chromatography

* Catalysis

* Enzymatic activity

Page 57: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The pioneering work of Gil-Av on

chiral separations of helicenes

E. Gil-Av, F. Mikes, G. Boshart, J. Chromatogr, 1976, 122, 205

A pair of enantiomers of a [6]-helicene

Silica derivatized with a chiral silylating agent

Page 58: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Enantioselectivity of a chiral chormatographic column

towards helicenes

Is there a relation between this behavior and the degree of chirality of helicenes?

Page 59: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The chiral separation of helicenes on Gil-Av’s column is dictated by their degree of chirality

O. Katzenelson Tetrahedron-Asymmetry, 11, 2695 (2000)

Gil-Av

Quantitative chirality

Page 60: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Catalysis

Page 61: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

N

OO

CH2

Cu N

X X

ON

O O

O N

OO

n

X = OTf

1 n = 12 n = 23 n = 34 n = 4

1-4

5 6

Catalytic Chiral Diels-Alder Reaction

Data: Davies, 1996. Analysis: Lipkowitz, Katzenelson

Page 62: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The nearest symmetry plane of the catalyst

n = 1

Page 63: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The enantiomeric excess of the product

as a function of the degree of chirality of the catalyst

Lipkowitz, JACS 123 6710 (2001)

Page 64: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

N

Cu

N

O O

C C

CC

SS

S1 S2

CC C

N

Cu

N

CC

O O

C

C

C

C

SO

O

CF

F F

SO

O

CF

F F

C C

CC

CC

N

Cu

N

O O

C

C

C

C

S

CF

F F

S

CF

F F

C

CC C

C

C

Sb Sg

Which smallest fragment carries the essential chirality?

S. Alvarez

Page 65: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The smallest fragment which carries

the essential chirality for catalysis

Page 66: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Prediction 1: Replace the exocyclic ring with C=O or C=CH2 to get good homologue catalysts

Page 67: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Prediction 2: Increase the twist angle

Page 68: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Enzymatic activity

Page 69: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Trypsin inhibitors

S. Keinan JACS 98

Page 70: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Attempt to find a correlation between the inhibition constant and the chirality of the whole inhibitor

No correlation; but…

Page 71: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The correlation follows the degree of chirality but not the length of the alkyl chain

Correlation between inhibition

and the chirality of the pharmacophor

Page 72: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Inhibition of acetylcholine esterase by chiral organophosphates

Page 73: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Ala82Asn83

Ile84

Gly50

HIV protease complexed

with A77 inhibitor

HIV protease-drug complex C2-symmetric color map

Page 74: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

F

FF

FFF

FF

FF

F

J

E

-16000

-15000

-14000

-13000

-12000

-11000

-10000

-9000

-8000

-5.0 -4.0 -3.0 -2.0 -1.0 0.0 1.0

G [

Kcal/

mol]

[S(C )]2

F: Native HIV-protease inhibitors

E: Native HIV-protease inhibitor A77

J: V82A mutant HIV-protease inhibitor A77

Free energy of inhibitors binding vs. their C2-symmetry change

Page 75: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Given a sufficiently high resolution in space or in time, nothing is symmetric, everything is chiral

Page 76: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

Our web-site (beta)

http://chirality.ch.huji.ac.il/ or http://www.csm.huji.ac.il/

Page 77: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 78: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 79: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 80: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 81: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 82: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013
Page 83: Continuous Symmetry and Chirality Measures David Avnir Institute of Chemistry The Hebrew University of Jerusalem Harvard, Boston, January 28, 2013

The J. Am. Chem. Soc. Series:

114, 7843 (1992)115, 8278 (1993)117, 462 (1995)120, 6152 (1998)122, 4378 (2000)123, 6710 (2001)125, 4368 (2003)126, 1755 (2004)

Literature

Recent:

A. Steinberg et al, "Continuous Symmetry Analysis of NMR Chemical Shielding Anisotropy”, Chem. Eur. J., 12, 8534 – 8538 (2006)

D. Yogev-Einot et al, "The temperature-dependent optical activity of quartz: from Le Chaˆtelier to chirality measures”, Tetrahedron: Asymmetry 17, 2723 – 2725 (2006)

Mark Pinsky et al, "Symmetry operation measures”, J. Comput. Chem., 2007