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Supporting Information for Ultrafast IR spectroscopy of short-lived transients formed by femtosecond UV excitation of cytosine derivatives Susan Quinn,* a Gerard W. Doorley, a Graeme W. Watson, a Alexander J. Cowan, b Michael W. George, b Anthony W. Parker,* c Kate L. Ronayne, c Michael Towrie c and John M. Kelly.* a a School of Chemistry and Centre for Chemical Synthesis and Chemical Biology, Trinity College, Dublin 2, Ireland; E-mail: [email protected] b School of Chemistry, University of Nottingham, University Park, Nottingham c Central Laser Facility, STFC Rutherford Appleton Laboratory, Chilton, Didcot, Oxfordshire, OX11 0QX, UK Contents Methods ps-TRIR measurements Computational calculations List of Figures and Tables Figure 1. ps-TRIR of 10 mM dCMP Figure 2. Kinetics of dCMP at selected delays Figure 3. ps-TRIR of 10 mM dCMP under acidic conditions Figure 4. B3LYP calculations using mCyt Figure 5. MP2 calculations using mCyt Figure 6. B3LYP calculations using dCMP Table 1. B3LYP calculated IR vibrational frequencies with mode assignment Supplementary Material (ESI) for Chemical Communications This journal is (c) The Royal Society of Chemistry 2007

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Page 1: Supporting Information for Ultrafast IR spectroscopy of

Supporting Information for

Ultrafast IR spectroscopy of short-lived transients formed by femtosecond UV excitation of cytosine derivatives

Susan Quinn,*a Gerard W. Doorley,a Graeme W. Watson,a Alexander J. Cowan,b Michael W. George,b Anthony W. Parker,*c Kate L. Ronayne,c Michael Towriec and John M. Kelly.*a a School of Chemistry and Centre for Chemical Synthesis and Chemical Biology, Trinity College, Dublin 2, Ireland; E-mail: [email protected]

b School of Chemistry, University of Nottingham, University Park, Nottingham c Central Laser Facility, STFC Rutherford Appleton Laboratory, Chilton, Didcot, Oxfordshire, OX11 0QX, UK

Contents Methods

ps-TRIR measurements

Computational calculations

List of Figures and Tables

Figure 1. ps-TRIR of 10 mM dCMP

Figure 2. Kinetics of dCMP at selected delays

Figure 3. ps-TRIR of 10 mM dCMP under acidic conditions

Figure 4. B3LYP calculations using mCyt

Figure 5. MP2 calculations using mCyt

Figure 6. B3LYP calculations using dCMP

Table 1. B3LYP calculated IR vibrational frequencies with mode assignment

Supplementary Material (ESI) for Chemical CommunicationsThis journal is (c) The Royal Society of Chemistry 2007

Page 2: Supporting Information for Ultrafast IR spectroscopy of

Methods

Ps-TRIR measurements. Measurements were performed at the PIRATE ultrafast

infrared absorption facility at the Rutherford Appleton Laboratory, Chilton which has

been described in detail elsewhere.1 Briefly, the sample was excited with 267-nm,

150-fs pulses with 2 μJ of energy at 0.5 kHz repetition rate, generated from the third

harmonic of part of the output from a 1kHz, 800 nm, 150 fs, 1 mJ regenerative

amplifier (Spectra Physics Tsunami/Spitfire) and probed with 150 cm-1 fwhm

broadband infrared pulses generated by difference frequency mixing the signal and

idler outputs of a BBO (β-BaB2O4) optical parametric amplifier, pumped with some

residual 800 nm, in AgGaS2 at 1 kHz. The spot size was 200 μm and 150 μm

diameter for the pump and the probe beam, respectively. The difference signal pump-

on minus pump-off was normalized on a shot-by-shot basis and typically accumulated

for four successive rounds of 30 s data integration for a single time delay. The

infrared beams were dispersed by 150 l/mm, 4000 nm blaze, gold grating

monochromators and imaged onto 64 element MCT array. The data were collected in

three 150 cm-1 spectral windows centred at 1646, 1552 and 1494 cm-1 using the delay

line for optical delays between 2 ps and 1 ns, normally at 2, 3, 4, 5, 6.5, 8, 10, 12.5,

15, 20, 35, 50, 100, 150, 200, 500, and 1000 ps. The difference signal was calibrated

using water lines present in the probe spectrum, and the spectral windows were

interleaved after scaling using overlapping transients recorded at the same delay time.

(This was done at 1554 cm-1 for dCyd, 1596 cm-1 for dCMP and at 1534 and 1585

cm-1 for Cyt.) The sample was raster scanned in x- and y- directions at an

approximate rate of 100 mm/ms.

1. M. Towrie, D. C. Grills, J. Dyer, J. A. Weinstein, P. Matousek, R. Barton, P. D. Bailey, N. Subramaniam, W. M. Kwok, C. S. Ma, D. Phillips, A. W. Parker and M. W. George, Applied Spectroscopy, 2003, 57, 367.

Computational Calculations. We have performed optimisations and vibrational

frequency calculations using both B3LYP and MP2 with a 6-311+G(2d,p) basis set in

the Gaussian 03 package. B3LYP and MP2 results are presented with all frequencies

scaled by a factor of 0.9679 and 0.9427 respectively. The simulated spectra are

obtained using the calculated intensity and a Gaussian distribution with a standard

deviation of 15 cm-1. To compare to experiment we have calculated the difference

Supplementary Material (ESI) for Chemical CommunicationsThis journal is (c) The Royal Society of Chemistry 2007

Page 3: Supporting Information for Ultrafast IR spectroscopy of

spectra between the tautomers and 1-methylcytosine (Figs 4 and 5) and between the

tautomers and dCMP (Fig 6).

Fig 1. (a) ps-TRIR of 10 mM dCMP in 50mM phosphate buffer pH 7, FTIR below (baseline adjusted) Delays –50, -25 (green), 2, 3, 4, 5, 6.5, 8 (red), 10, 15, 20, 35, 50, 100, 500 and 1000 ps (black).

Wavenumber (cm-1)

1500 1550 1600 1650 1700

Cha

nge

in A

bsor

banc

e

-0.0015

-0.0010

-0.0005

0.0000

0.0005

Supplementary Material (ESI) for Chemical CommunicationsThis journal is (c) The Royal Society of Chemistry 2007

Page 4: Supporting Information for Ultrafast IR spectroscopy of

Fig 2. Kinetic analysis of 10 mM dCMP in 50 mM phosphate buffer pH 7 at 1574 and 1649 cm-1

Fig 3. ps-TRIR of 10 mM dCMP under acidic conditions, 0.132 M H3PO4 in D2O, and inset kinetics recorded at 1658 cm-1. Delays at –50, -25 (green), 2, 3, 4, 5, 6.5, 8 (red), 10, 15, 20, 35, 50, 100, 500 and 1000 ps (black).

Wavenumber (cm-1)1550 1600 1650 1700

Cha

nge

in A

bsor

banc

e

-0.0015

-0.0010

-0.0005

0.0000

0.0005

0 10 20 30 40 50 60

-0.0012

-0.0008

-0.0004

0.0000

Carbonyl stretch 1658 cm-1

t1= 4.0 (0.4)ps

Cha

nge

in A

bsor

banc

e

Time ps

0 200 400 600 800 1000

-0.0010

-0.0005

0.0000

0.0005

dCMP 1574 cm-1

dCMP 1649 cm-1

Cha

nge

in A

bsor

banc

e

Time (ps)

Supplementary Material (ESI) for Chemical CommunicationsThis journal is (c) The Royal Society of Chemistry 2007

Page 5: Supporting Information for Ultrafast IR spectroscopy of

Fig 4. B3LYP Calculations (a) Calculated IR spectra of mCyt and tautomers I and H, and (b) difference spectra of tautomer I compared to mCyt, tautomer H compared to mCyt and experimental data for dCyd at 10 ps. (with both predicted spectra having a scaling factor of 0.96790 applied)

1400 1450 1500 1550 1600 1650 1700 1750Wavenumber (cm-1)

mCyt Tautomer I Tautomer H

1400 1450 1500 1550 1600 1650 1700 1750

Wavenumber (cm-1)

Tautomer I - mCyt Tautomer H - mCyt dCyd 10 ps delay

(a)

(b)

Supplementary Material (ESI) for Chemical CommunicationsThis journal is (c) The Royal Society of Chemistry 2007

Page 6: Supporting Information for Ultrafast IR spectroscopy of

Fig 5. MP2 Calculations (a) Calculated IR spectra of mCyt and tautomers I and H, and (b) difference spectra of tautomer I compared to mCyt, tautomer H compared to mCyt and experimental data for dCyd at 10 ps. (with both predicted spectra having a scaling factor of 0.9427 applied)

1400 1450 1500 1550 1600 1650 1700 1750

Wavenumber (cm-1)

mCyt Tautomer I Taoutomer H

1400 1450 1500 1550 1600 1650 1700 1750

Wavenumber (cm-1)

Tautomer I - mCyt Tautomer H - mCyt dCyd 10 ps delay

(a)

(b)

Supplementary Material (ESI) for Chemical CommunicationsThis journal is (c) The Royal Society of Chemistry 2007

Page 7: Supporting Information for Ultrafast IR spectroscopy of

Fig 6. B3LYP Calculations (a) Calculated IR spectra of dCMP and tautomers I and H, and (b) difference spectra of tautomer I compared to dCMP, tautomer H compared to dCMP and experimental data for dCMP at 10 ps. (with both predicted spectra having a scaling factor of 0.96790 applied)

1400 1450 1500 1550 1600 1650 1700 1750

Wavenumber (cm-1)

dCMP Tautomer I Tautomer H

1400 1450 1500 1550 1600 1650 1700 1750Wavenumber (cm-1)

Tautomer I - dCMP Tautomer H - dCMP dCMP 10 ps delay

(a)

(b)

Supplementary Material (ESI) for Chemical CommunicationsThis journal is (c) The Royal Society of Chemistry 2007

Page 8: Supporting Information for Ultrafast IR spectroscopy of

mCyt (cm-1)

Principal Components

Tautomer I (cm-1)

Principal Components

Tautomer H (cm-1)

Principal Components

1678

C2-O 1700 N3-C2,

1656 C5-C6, C2-N3

1621

C5-C6, C4-NH2

1633 C5-C6,

C4-NH 1596 C4-NH,

C2-N3

1505 C4-C5

C5-C1 C4-NH2

1566 C4-NH, C5-C6

1531

C4-NH, C2-N3 C5-C6

Table 1. B3LYP calculated IR vibrational frequencies with principal mode assignment. A Scaling factor of 0.96790 has been applied to all frequencies.

N

N

N

O

CH3

HH

N

N

N

O

CH3

H

HN

N

N

HO

CH3

H

(C) (I) (H)

32 1

4 5

6

Supplementary Material (ESI) for Chemical CommunicationsThis journal is (c) The Royal Society of Chemistry 2007