the pure rotational spectrum of ticl + (x 3 r ) by velocity modulation spectroscopy dewayne t....

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The Pure Rotational Spectrum of TiCl + (X 3 r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department of Astronomy Steward Observatory Arizona Radio Observatory University of Arizona June 21, 2004

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Page 1: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

The Pure Rotational Spectrum of TiCl+ (X3r) by Velocity Modulation Spectroscopy

DeWayne T. Halfen and Lucy M. Ziurys

Department of ChemistryDepartment of Astronomy

Steward ObservatoryArizona Radio Observatory

University of Arizona

June 21, 2004

Page 2: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

Why Molecular Ions ?Why Molecular Ions ?

• Chemical Aspect– Organic intermediates

– Stratospheric chemistry

– Combustion chemistry

• Astronomical Aspect– Many molecular ions in

interstellar medium

• Radicals – Difficult to study– Few molecular ions studied at

high resolution

Ions Studied at High Resolution

H3+ CO+ CH +

SO+ HCO+ HOC+

H2D+ HCS+ N2H+

H3O+ CH2D+ HCNH+

HOCO+ H2COH+ HC3NH+

OH+ OH HCl+

ArH+ HBr+

• Neutral species dominate over ions

• Built a new spectrometer – uses Velocity Modulation– Ion selective technique

Page 3: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

Velocity Modulation SpectrometerVelocity Modulation Spectrometer

Page 4: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

Detector

RadiationSource

Gas Cell

Reactant

Page 5: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

Characteristics of Velocity ModulationCharacteristics of Velocity Modulation

• Drift velocity of TiCl+

– E = 1.9 V/cm, (Ar) = 1.6411 Å3, (Ar-TiCl+) = 26.99 amu, T = 208 K, P = 50 mTorr

– vd = 458.8 m/s

• Doppler shift

– = 606 kHz at v0 = 396 GHz

• Line width: ~ 1300 kHz

• Modulation index = / = 0.46– Under-modulated at millimeter wavelengths

15.273

T

P

760876.13Ev

2/1d

c

vvδν d

0

Page 6: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

413.38 413.40 413.42 413.44 413.46 413.48

Frequency (GHz)

Source Modulation

46Ti35Cl+ ( = 2)J = 38 39

Source Modulation

413.38 413.40 413.42 413.44 413.46 413.48

Frequency (GHz)

Velocity Modulation

46Ti35Cl+ ( = 2)J = 38 39

Velocity Modulation

412.76 412.78 412.80 412.82 412.84

Frequency (GHz)

Source Modulation

48Ti35Cl ( = 7/2)J = 41.5 42.5

Source Modulation

412.76 412.78 412.80 412.82 412.84

Frequency (GHz)

Velocity Modulation

48Ti35Cl ( = 7/2)J = 41.5 42.5

Velocity Modulation

382.56 382.58 382.60 382.62 382.64

Frequency (GHz)

Source Modulation

V35Cl ( = 0e)J = 38 39

Source Modulation

382.56 382.58 382.60 382.62 382.64

Frequency (GHz)

Velocity Modulation

V35Cl ( = 0e)J = 38 39

Velocity Modulation

• <5% leakage of neutral signals in VM mode

Using Velocity ModulationUsing Velocity Modulation

• Use velocity modulation to distinguish neutrals from ions

Page 7: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

Past Studies of TiCl+Past Studies of TiCl+

• Balfour & Chandrasekhar (1990)– First observed visible spectrum

• Kaledin & Heaven (1995,1997a,1997b) – Predicted X3r & confirmed using laser absorption

• Focsa et al. (1997a,1997b,1998,1999)– Used laser absorption/velocity modulation to measure several

electronic transitions

– Found that the = 2 & 3 subbands of X3r perturbed by 3r state

– Established spectroscopic constants for each state

Page 8: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

Gas-Phase Synthesis of TiCl+Gas-Phase Synthesis of TiCl+

• Add TiCl4

– Pressure: <1 mTorr

• 20 mTorr Ar gas also added

• AC discharge – 200 W at 600

Page 9: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

Energy Level Diagram for TiCl+Energy Level Diagram for TiCl+

• 3r ground state– Two unpaired 3d electrons

• J = L + S

• Spin-orbit and spin-spin interactions– &

• Omega ladders– = 2, 3, 4

– J ≥

• A3r state close in energy– Perturbs = 2 & 3 ladders

SLAH so SSH ss

0

100

200

300

400

500

600

700

En

erg

y (

cm

-1)

A3r

= 4

= 3

= 2: v = 0

= 1

= 2

= 3

X3r

Page 10: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

395.945 395.965395.64 395.66Frequency (GHz)

396.095 396.115

48Ti35Cl+ (X3r): J = 37 38 = 2

= 4

= 3

Source Modulation

395.945 395.965395.640 395.660Frequency (GHz)

396.095 396.115

48Ti35Cl+ (X3r): J = 37 38 = 2

= 4 = 3

Velocity ModulationVelocity Modulation

392 393 394 395 396Frequency (GHz)

TiCl+ (X3r) = 2

= 3

= 4

48Ti35Cl+

J = 37 38

46Ti35Cl+

J = 36 37

48Ti37Cl+

J = 38 39

Rotational Spectrum of TiCl+Rotational Spectrum of TiCl+

• Fine structure components shifted from normal pattern

• TiCl+ confirmed by VM– S/N down by

factor of 4

• Measured 37Cl, 46Ti isotopomers in natural abundance

Page 11: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

• Measured 10 rotational transitions of 48Ti35Cl+, 48Ti37Cl+, & 46Ti35Cl+

J J obs obs - calc J J obs obs - calc

30 31 2 322927.414 -0.015 35 36 2 374883.903 -0.009

3 323297.905 -0.089 3 375315.282 0.021

4 323156.037 -0.081 4 375163.298 0.063

31 32 2 333322.960 0.013 36 37 2 385268.555 -0.001

3 333705.663 0.028 3 385712.131 0.015

4 333561.278 -0.035 4 385558.787 0.053

32 33 2 343716.434 0.015 37 38 2 395650.832 -0.001

3 344111.266 0.020 3 396106.617 -0.007

4 343964.669 -0.011 4 395952.103 0.025

33 34 2 354107.777 -0.003 38 39 2 406030.676 -0.003

3 354514.788 0.025 3 406498.708 -0.014

4 354366.190 0.029 4 406343.266 -0.003

34 35 2 364496.962 -0.003 39 40 2 416408.036 0.006

3 364916.143 0.021 3 416888.324 -0.021

4 364765.753 0.055 4 416732.131 -0.099

Rest Frequencies of 48Ti35Cl+ (X3r)Rest Frequencies of 48Ti35Cl+ (X3r)

Page 12: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

Spectroscopic Analysis of TiCl+Spectroscopic Analysis of TiCl+

• Determined spectroscopic constants for TiCl+

sssoroteff HHHH

48Ti35Cl+

Parameter MMW Optical

B 5216.6676(21) 5226.07(54)

D 0.00256353(78) 0.002728(45)

A 1900000 a 1904570(80)

AD 2.7834(89) -0.489(54)

AH 6.308(36) x 10-5

4404278(5000) 11030(180)

D -18.071(46) 0.507(18)

H -1.000 x 10-5 a

rms 0.037 a Held Fixed

• Rotational constants agree

• Fine structure parameters different– Different analysis

methods

• reflects large perturbation from A3r state

Page 13: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

TiCl vs. TiCl+TiCl vs. TiCl+

• Relative intensities of TiCl vs. TiCl+ very similar

• Neutral only ~1.5x stronger than ion

• Ions usually very small fraction of plasma

• TiCl4 produces ions well

406.023 406.043

-0.5

0.0

0.5

1.0

Frequency (GHz)393.456391.298

-0.5

0.0

0.5

1.0

394.554392.375

406.334 406.354 406.491 406.511

= 3 = 4

= 2

48Ti35Cl (X4r): J = 39.5 40.5

48Ti35Cl+ (X3r): J = 38 39

*

= 3/2

= 5/2

= 7/2 = 9/2In

tens

ity

(mV

)In

tens

ity

(mV

)

Page 14: The Pure Rotational Spectrum of TiCl + (X 3  r ) by Velocity Modulation Spectroscopy DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department

Future WorkFuture Work

408.78 408.80 408.82 408.84 408.86

Frequency (GHz)

TiN (X2+)N = 10 11

J = 10.5 11.5

J = 9.5 10.5

• Measure spectra of more titanium species & molecular ions– TiC (X3), TiN+ (X1+), TiO+ (X2r), TiF+ (X3r)

411.39 411.41 411.43 411.45 411.47

Frequency (GHz)

TiO (X3r)

J = 12 13 = 1e/f

* *

• VCl - TH11

• VCl+ - TH12