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Juraj Varga - Prof. Per Jensen, Ph.D.

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<strong>Juraj</strong> <strong>Varga</strong><br />

FSO 3 • radical measurements and improvements of our spectrometer<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


Laboratory of High Resolution Molecular Spectroscopy<br />

Prague<br />

‣ QUASAAR fellow from the 1 st January 2007 in the Laboratory of High Resolution Molecular<br />

Spectroscopy in Prague<br />

‣ research activities of the laboratory - high resolution spectroscopy in microwave spectral region<br />

of radicals and halogen containing molecules of an atmospheric importance i<br />

and their<br />

theoretical analysis → extremely accurate molecular structure and electrodynamical parameters<br />

‣ measurement of precise ground state rotational frequencies of stable molecules - CH 3 Br and<br />

radicals FCO 2 •,, FSO 3 •<br />

‣ L. Kolesniková, , J. <strong>Varga</strong>, H. Beckers, , M. Šimečková, , Z. Zelinger, , L. Nová Střítesk<br />

teská, , P. Kania, , H. Willner, and Š.<br />

Urban: Detailed study of fine and hyperfine structures in rotational spectra of the free fluoroformyloxyl radical<br />

FCO2, J. Chem. <strong>Ph</strong>ys. . 128, 1-8, 1<br />

(2008).<br />

‣ L. Kolesniková, , J. <strong>Varga</strong>, L. Nová Střítesk<br />

teská, , H. Beckers, , H. Wilner, , F. Aubke, and Š. . Urban: The Ground State<br />

Rotational Spectrum of the Fluorosulfate Radical, , J. Chem. <strong>Ph</strong>ys.,<br />

Accepted 2009.<br />

‣ improvement of measurements - development of the different modulation systems – Stark and<br />

Zeeman modulation<br />

‣ other experiments – multireflexion cell for weak transitions, Fabry-<strong>Per</strong>ot resonator for low<br />

frequencies (2-50 GHz)<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


Laboratory of High Resolution Molecular Spectroscopy<br />

Prague<br />

The Prague millimeterwave spectrometer setup with the pyrolysis device for radical measurements.<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


FSO 3<br />

• radical<br />

‣ the fluorosulfate radical – open shell system with one unpair electron → primarily causes a fine<br />

splitting of the rotational levels into two sublevels – eletron spin-rotational interaction<br />

‣ magnetic hyperfine interactions between the magnetic moments of the open shell electron<br />

system and the 19 F nucleus as well as nuclear spin-rotational interaction → additional hyperfine<br />

doubling of levels – very small, in rotational spectra nearly unresolved<br />

‣ radical was produced by a low pressure pyrolysis of the bis(fluorosulfuryl)peroxide (430 K,<br />

sample pressure of the equilibrium mixture was 6 ubar)<br />

FSO 2 O-OSOOSO 2 F ↔ 2 FSO3•<br />

‣ measurements spectral range – 93-281 GHz, frequency modulation with the second harmonic<br />

lock-in detection<br />

‣ measured in its vibronic ground state, more than 250 fine rotational transitions have been<br />

en<br />

observed, analyzed in detail using the matrix elements of the rotational, fine and hyperfine<br />

Hamiltonian terms – observed, identified and analyzed for the first time<br />

‣ derived very precise values of the rotational, centrifugal distorsion and fine constants and the<br />

C 3v molecular symetry of the vibronic ground state was unambigously confirmed<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


FSO 3<br />

• radical<br />

0.0007<br />

0.0006<br />

0.0005<br />

0.0004<br />

0.0003<br />

intensity [a.u.]<br />

0.0002<br />

0.0001<br />

0.0000<br />

-0.0001<br />

-0.0002<br />

-0.0003<br />

-0.0004<br />

-0.0005<br />

270000 272000 274000 276000 278000 280000<br />

frequency [MHz]<br />

10 GHz overview with 150 MHz step – ~ 1000 lines, ~ 30 belongs to FSO3• radical<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


FSO 3<br />

• radical<br />

0.00004<br />

intensity [a.u.]<br />

0.00000<br />

269970 270000 270030<br />

frequency [MHz]<br />

Example of the spectrum of fluorosulfate radical rotational transition N’ ← N” =26← 25<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


FSO 3<br />

• radical<br />

The radical and nonradical spectra measured with and without the magnetic field: a) the radical<br />

lines are broadened and their peak heights are decreased because of the molecular Zeeman<br />

Effect; b) the lines of the closed shell molecules are unaffected by the magnetic field and both the<br />

spectrum traces are completely overlapped<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


FSO 3<br />

• radical<br />

The simple Loomis–Wood diagram indicates the assignments of the radical transition lines to rotational and<br />

electron spin quantum numbers. The two groups of points for a given upper N’ quantum number correspond to<br />

different values of ms = ±½ and thus to different components of the fine splitting. For some of these groups, the<br />

highest possible K values are indicated.<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


FSO 3<br />

• radical<br />

The parts of the radical spectrum with transitions from energy<br />

levels with the quantum numbers N” = 19 in the vibronic ground<br />

state corresponding to the row with N’ = 20 of the Loomis–Wood<br />

diagram<br />

An illustration of the resolved hyperfine<br />

splitting in the fluorosulfate radical rotational<br />

transition N’ ← N” =10← 9.<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


FSO 3<br />

• radical<br />

The molecular parameters of the fluorosulfate radical in the vibronic ground state a,b,c .<br />

Parameter<br />

without hyperfine splitting<br />

with hyperfine splitting<br />

B<br />

5195.528365 (259)<br />

5195.528364 (291)<br />

D N<br />

×10 3 3.76291 (60)<br />

3.76287 (64)<br />

D NK<br />

×10 3 −1.28189 (131)<br />

−1.28162 (183)<br />

H N<br />

×10 9 −6.75 (44)<br />

−6.83 (46)<br />

H NK<br />

×10 6 0.18816 (127)<br />

0.18872 (156)<br />

H KN<br />

×10 6 −0.34627 (194)<br />

−0.34765 (307)<br />

h 3<br />

×10 9 6.640 (21) b<br />

6.640 (21) b<br />

ε aa<br />

−37.372 (59)<br />

−37.344 (67)<br />

ε bb<br />

−271.9178 (189)<br />

−271.8446 (265)<br />

D S N ×103 −0.9931 (73)<br />

−1.0123 (90)<br />

D S NK<br />

−0.0696 (188)<br />

−0.0616 (228)<br />

D S KN<br />

0.0725 (190)<br />

0.0646 (230)<br />

D S K ×103 −1.628 (275)<br />

−1.58 (37)<br />

a F<br />

…<br />

−24.1 (45)<br />

1.5 T aa<br />

…<br />

−2.628 (288)<br />

s c 0.014<br />

0.014<br />

a All the data are in MHz. The numbers in parentheses<br />

are standard deviations in the units of the last decimal<br />

digit. The frequencies of the K = 3 doublets are<br />

averaged.<br />

b Fitted separately.<br />

c The symbol s denotes a standard deviation of the fit.<br />

‣L.<br />

Kolesniková, , J. <strong>Varga</strong>, L. Nová Střítesk<br />

teská, , H. Beckers, , H.<br />

Wilner, , F. Aubke, and Š. . Urban: The Ground State Rotational<br />

Spectrum of the Fluorosulfate Radical, , J. Chem. <strong>Ph</strong>ys.,<br />

Accepted 2009.<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


Stark modulation<br />

f [kHz]<br />

U in [V]<br />

1<br />

2<br />

4<br />

6<br />

8<br />

10<br />

12<br />

14<br />

16<br />

18<br />

20<br />

22<br />

24<br />

26<br />

28<br />

30<br />

32<br />

34<br />

36<br />

38<br />

40<br />

44<br />

46<br />

50<br />

3150<br />

3100<br />

3050<br />

3000<br />

2900<br />

2740<br />

2600<br />

2450<br />

2400<br />

2400<br />

2400<br />

2400<br />

2370<br />

2350<br />

2200<br />

1800<br />

1250<br />

1100<br />

1075<br />

1000<br />

1000<br />

1000<br />

1000<br />

975<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


Zeeman modulation<br />

Modulation frequency 0.5 – 3 kHz, magnetic field 4 mT<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


Acknowledgement<br />

‣ Marie Curie Research Training Network (QUASAAR)<br />

‣ <strong>Prof</strong>. RNDr. Štěpán Urban, CSc. as my supervisor<br />

‣ all collaborating laboratories: Wuppertal - prof. Willner group, CTU Prague<br />

QUASAAR Winter School, February 20-25, 25, 2009 Demänovsk<br />

novská Dolina - Jasná, , Slovakia


Laboratory of High Resolution Molecular Spectroscopy<br />

Prague<br />

<strong>Prof</strong>. RNDr. Štěpán Urban, CSc.<br />

Ing. Lucie Nová – Stříteská, <strong>Ph</strong>D.<br />

Ing. Lucie Kolesníková<br />

Ing. Patrik Kania, <strong>Ph</strong>D.<br />

Ing. Jindřich Koubek<br />

Michal Rybníček<br />

Mgr. Tereza Uhlíková, <strong>Ph</strong>D.<br />

juraj.varga@vscht.cz<br />

http://www.vscht.cz/anl/lmsvr/


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