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Items: 1 to 20 of 303

1.

The NaK 1(b) 3Pi(Omega=0) state hyperfine structure and the 1(b) 3Pi(Omega=0) approximately 2(A) 1Sigma+ spin-orbit interaction.

Burns P, Wilkins AD, Hickman AP, Huennekens J.

J Chem Phys. 2005 Feb 15;122(7):074306.

PMID:
15743231
2.

Experimental study of the NaK 3 3Pi double minimum state.

Morgus L, Burns P, Miles RD, Wilkins AD, Ogba U, Hickman AP, Huennekens J.

J Chem Phys. 2005 Apr 8;122(14):144313.

PMID:
15847528
3.

The Na2 2 3pi(g) state: new observations and hyperfine structure.

Qi P, Lazarov G, Lyyra AM, Liu Y, Cui C, Li L, Jeung GH.

J Chem Phys. 2006 May 14;124(18):184304.

PMID:
16709103
4.

The NaK 1 1,3delta states: theoretical and experimental studies of fine and hyperfine structure of rovibrational levels near the dissociation limit.

Wilkins AD, Morgus L, Hernandez-Guzman J, Huennekens J, Hickman AP.

J Chem Phys. 2005 Sep 22;123(12):124306.

PMID:
16392481
5.

Nonadiabatic coupling in the 3 3Pi and 4 3Pi states of NaK.

Miles RD, Morgus L, Kashinski DO, Huennekens J, Hickman AP.

J Chem Phys. 2006 Oct 21;125(15):154304.

PMID:
17059252
6.
7.

Hyperfine structures of the 2 (3)Sigma(g) (+), 3 (3)Sigma(g) (+), and 4 (3)Sigma(g) (+) states of Na(2).

Liu Y, Li L, Lazarov G, Lazoudis A, Lyyra AM, Field RW.

J Chem Phys. 2004 Sep 22;121(12):5821-7.

PMID:
15367008
9.

Fine structure and hyperfine perturbations in the pure rotational spectrum of the VCl radical in its X 5Delta(r) state.

Halfen DT, Ziurys LM, Brown JM.

J Chem Phys. 2009 Apr 28;130(16):164301. doi: 10.1063/1.3108538.

PMID:
19405573
10.

The A (3Pi1) State of ClF.

Alekseev VA, Setser DW, Tellinghuisen J.

J Mol Spectrosc. 1999 May;195(1):162-171.

PMID:
10191161
11.

Ab initio study including spin-orbit effects on the B-X transition of AgI.

Ramirez-Solis A.

J Chem Phys. 2004 Feb 1;120(5):2319-24.

PMID:
15268370
12.

Ab initio study on the ground and low-lying excited states of cesium iodide (CsI).

Kurosaki Y, Matsuoka L, Yokoyama K, Yokoyama A.

J Chem Phys. 2008 Jan 14;128(2):024301. doi: 10.1063/1.2821103.

PMID:
18205444
13.
14.

Perturbations in the pure rotational spectrum of CoCl (X 3 Phi i): a submillimeter study.

Flory MA, Halfen DT, Ziurys LM.

J Chem Phys. 2004 Nov 1;121(17):8385-92.

PMID:
15511159
15.

The 4(3)Pi(g) State of Na(2): Vibrational Numbering and Hyperfine Structure.

Lazarov G, Lyyra AM, Li L, Huennekens J.

J Mol Spectrosc. 1999 Aug;196(2):259-264.

PMID:
10409455
16.

The rotational spectrum of CoF in all three spin-orbit components of the X3Phi i state.

Harrison JJ, Brown JM, Flory MA, Sheridan PM, McLamarrah SK, Ziurys LM.

J Chem Phys. 2007 Nov 21;127(19):194308.

PMID:
18035884
17.

Rotational spectrum and carbon-13 hyperfine structure of the C3H, C5H, C6H, and C7H radicals.

McCarthy MC, Thaddeus P.

J Chem Phys. 2005 May 1;122(17):174308.

PMID:
15910033
18.

The spin-orbit and rotational constants for the N2 C" 5Pi(ui) (v = 3) state.

Field RW, Pirali O, Tokaryk DW.

J Chem Phys. 2006 Feb 28;124(8):081103.

PMID:
16512697
19.

Hyperfine interaction and Stark effect in the b 3Pi-X 1Sigma+(0,0) band of copper monofluoride, CuF.

Wang F, Steimle TC.

J Chem Phys. 2010 Feb 7;132(5):054301. doi: 10.1063/1.3292606.

PMID:
20136310
20.

Electronic spectrum of AuF: hyperfine structure of the [17.7]1 state.

Knurr BJ, Butler EK, Varberg TD.

J Phys Chem A. 2009 Nov 26;113(47):13428-35. doi: 10.1021/jp904472y.

PMID:
19921947

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