EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban...

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EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia

Transcript of EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban...

Page 1: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

EII of plasma edge constituents, properties of BexHy molecules

S. Matejcik, P. Mach, J. Urban

Comenius UniversityBratislavaSlovakia

Page 2: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Bratislava

Page 3: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Overview

- Appearance energies of C2D6

- Cross section for EII to propane

- BeH and BeH2 – structure and energies

- Structure and energetics of BemHn clusters

Page 4: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Electron impact ionization

cross sections (total, partial) ionization energies appearance energies kinetic energy release gas temperature dependencies products of the reactions

Page 5: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Experimental setup

Page 6: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Cross section measurements

Absolute measurement of the pressure

Relative flow technique

Ar as a calibration gas

Page 7: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Atoms:

Wannier theory:

w(E,AE,A,d) = 0 E<AE A(E-IE)d E>AEd=1.127

Threshold behaviour of the cross sections

dEUEfAdAEEAdAEEI w ),(),,,(),,,(0

f(E,U) - EEDF

Fitting function:

Page 8: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

23,5 24,0 24,5 25,0 25,5

0

100

200

300

400

500

He+/He

Ion

yiel

d (a

rb.

units

)

E (eV)

d=1.127±0.01

Threshold behaviour of the cross sections

Page 9: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

CH3D

AE (eV)293 K

CD4

AE (eV)293 K

CH4

AE (eV)293 K

CH3D+ 12.75 ± 0.03 12.89 ± 0.03 12.65 ± 0.04 CH4

+

CH2D+ + H–

CH2D+ + H

13.66 ± 0.07 14.42 ± 0.05

- 14.54 ± 0.05

13.58 ± 0.1 14.34 ± 0.1

CH3+ + H–

CH3+ + H

Isotopic effect on AE

Denifl et al. IJMS 248 (2005) 29

Page 10: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

PresentmeV

a)meV

b)meV

(CH3D)+/CH3D 100 50

(CH2D)+/CH3D 80

(CH3)+/CH3D 200

(CHD)+/CH3D 110

(CD4)+/CD4 190 170 160

(CD3)+/CD4 200 130

(CD2)+/CD4 310 90

a) F. P. Lossing, A. W. Tickner, W. A. Bryce, J. Chem. Phys. 19, 1254 (1951).b) V. H. Dibeler, M. Krauss, R. M. Reese, F. N. Harlee J. Chem. Phys. 42, 3791 (1965).

Isotopic shift

Denifl et al. IJMS 248 (2005) 29

Page 11: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

EII of C2D6

e + C2D6 → C2D6+ + 2e

→ C2D5+ + D– + 2e

→ C2D2+ + 2D2 + e

Page 12: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

EII to C2D6

11,0 11,5 12,0 12,5 13,0 13,5-1000

0

1000

2000

3000

4000

5000

6000

7000

8000Io

n S

igna

l (ar

b. u

nits

)

Electron energy (eV)

C2D

6

+ / C2D

6

11.46 eV

Page 13: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Izotopic effects in C2D6

aE. Vaseková, M. Stano, S. Matejcik, , J.D. Skalný, P. Mach, T.D. Märk, J. UrbanInt. J. of Mass Spect., 235 (2004) 155-162

e + C2D6 → AE (in eV)

Present Ethana

( C2D6 )+ 11.80 ± 0.05 11.46 ± 0.06

( C2D5 )+ 11.78 ± 0.07 ? 12.06± 0.03

( C2D4)+ 12.09 ± 0.08 11.9± 0.04

( C2D2)+ 15.06± 0.2 15.02± 0.2

Page 14: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Grill et al. ZPhysD 25 (1993) 217

Page 15: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

EII to C3H8

10 11 12 13

0

2x10-19

4x10-19

6x10-19

8x10-19

Ion

yie

ld (

arb

. Un

its)

E (eV)

C2H

+ 5/C

3H

8

C3H

+ 8/C

3H

8

C2H

+ 4/C3H

8

C3H

+ 7/C

3H

8

Page 16: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Appearance energies C3H8

Denifl CPL 402 (2005) 80

Page 17: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

EII to C3H8 cross sections

Exp: N. Duric, I. Čadež, M. Kurepa, Int. J. Mass Spectrom. & Ion Processes, 108 (1991) R1-R10.

9,5 10,0 10,5 11,0 11,5 12,0 12,5 13,0 13,5 14,0

0,0

2,0x10-17

4,0x10-17

6,0x10-17

C2H

+

5/C

3H

8

C3H+

7/C

3H

8

C2H+

4/C

3H

8

C3H

+

8/C

3H

8

Cro

ss S

ect

ion

[cm

2 ]

Electron Energy [eV]

Page 18: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Total cross sections

σBEB(12 eV) σPresent(12 eV) σExp(12 eV)

[10-16 cm2]

0.119 0.21 0.35

Exp: N. Duric, I. Čadež, M. Kurepa, Int. J. Mass Spectrom. & Ion Processes, 108 (1991) R1-R10.

BEB: W. Hwang, Y.-K. Kim and M.E. Rudd, J. Chem. Phys., 104 (1996) 2956

Page 19: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Cross sections at 700 K

Not finnished yet Problems with contamination

Page 20: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

EII to BexHy

Experimental problems

Vaporisation only at T>1000°C

Toxicity of Be

Page 21: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

BeH dissoc. energy

Roo

sAT

Z

Best Theor.

1.9

2.0

2.1

2.2

2.3

2.4

2.5

2.6D

e [e

V]

MP2(FC) MP2(Full)

CCSD(t,FC) CCSD(t,Full)

cc-pvXZ aug-cc-pvXZ cc-pCvXZ aug-cc-pCvXZ

CCSDT-R12

1exc. energy 2Σ – 2Π, experiment 17086 cm-1 , theory – 17116 cm-1

Page 22: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

BeH bond lenght

X=3

X=2

X=3

X=4

X=5

Roo

sAT

Z

X=5X=4

X=3

X=2

X=2

X=5

X=4

X=5

X=4

X=3

X=2

R12-CCSD(T)

1.310

1.315

1.320

1.325

1.330

1.335

1.340

1.345

1.350

1.355

1.360

Be-

H [

A]

MP2(FC)

MP2(Full)

CCSD(t,FC)CCSD(t,Full)

aug-cc-pCvXZcc-pCvXZaug-cc-pvXZcc-pvXZ

Page 23: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

BeH2

basis BeH2

Be-H [A]

TAEa)

[eV]DEBe+H2 [eV]

CCSD(T)-R12

Be:19s14p8d6f4gH: 9s,6p,4d,3f

1.3260 6.418 1.671

CCSD(T) Full

aug-cc-pCvDZ 1.3366 6.108 1.585

aug-cc-pCvTZ 1.3298 6.321 1.614

aug-cc-pCvQZ 1.3267 6.391 1.657

aug-cc-pCv5Z 1.3263 6.406 1.664

B3LYP6-311++G(3d,3p) 1.3248 6.741 1.965

aug-cc-pCv5Z 1.3239 6.748 1.964

Page 24: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

BeH2 bond lenght

R12-CCSD(T)

1.315

1.320

1.325

1.330

1.335

1.340

1.345

Be-

H [

A]

MP2(FC)

MP2(Full)

CCSD(t,FC)

CCSD(t,Full)

aug-cc-pvXZ aug-cc-pCvXZcc-pvXZ cc-pCvXZ

Page 25: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

BenH clusters – MP2

Page 26: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

BenH1

0

2

4

6

8

10

12

1 2 3 4 5

Number of Beryllium Atoms

En

erg

y [e

V]

Energy Difference

Atomization Energy

Page 27: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Be3Hn

Be4Hn

Page 28: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Be4Hn

0

5

10

15

20

25

30

35

0 1 2 3 4 5 6 7 8 9

Number of Hydrogen Atoms

En

erg

y D

iffe

ren

ce

[e

V]

Energy Difference

Atomization Energy

Page 29: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Futher plans

Propane cross section at high T C2D6 – high T, cross sections Ionization energies of the Be compounds Appearance energies of the fragments Simulation of the Be surface Chemistry on the Be surface

Page 30: EII of plasma edge constituents, properties of Be x H y molecules S. Matejcik, P. Mach, J. Urban Comenius University Bratislava Slovakia.

Thank you for your attention