+ All Categories
Home > Documents > Tunable Diode Laser Spectroscopy Application for Detection ... · Tunable Diode Laser Spectroscopy...

Tunable Diode Laser Spectroscopy Application for Detection ... · Tunable Diode Laser Spectroscopy...

Date post: 22-May-2018
Category:
Upload: ngoquynh
View: 221 times
Download: 1 times
Share this document with a friend
16
Tunable Diode Laser Spectroscopy Application for Detection and Isotopes Ratio Measurements of UF 6 Molecules. A.Nadezhdinskii, Ya.Ponurovskii, Yu.Shapovalov, D.Stavrovskii NSC of A.M.Prokhorov General Physics Institute D. Bolyasov, G.Grigoriev, S.Malyugin, Sh.Nabiev, N.Gorshunov Institute of Molecular Physics of RRC "Kurchatov Institute"
Transcript

Tunable Diode Laser Spectroscopy Application for Detection and Isotopes Ratio

Measurements of UF6 Molecules.

A.Nadezhdinskii, Ya.Ponurovskii, Yu.Shapovalov, D.Stavrovskii

NSC of A.M.Prokhorov General Physics Institute D. Bolyasov, G.Grigoriev, S.Malyugin, Sh.Nabiev,

N.Gorshunov Institute of Molecular Physics of RRC "Kurchatov Institute"

Introduction

Beginning of Tunable Diode Laser Spectroscopy (TDLS) was related to one molecule practically in all countries. It was UF6 molecule with respect to laser uranium isotopes separation. Dramatic progress in TDLS technique achieved during last decades and success of detection of trace complex molecules again brought our intention to the same molecule because of IAEA needs related to Additional Protocol of Safeguards. There were three objectives of present paper:

1. To investigate if it is possible to use Tunable Diode Laser Spectroscopy (TDLS) technique for gaseous uranium hexafluoride enrichment measurement.

2. To analyze possibility to detect trace UF6 presence in atmosphere. 3. To detect trace HF molecule concentration due to hydrolysis of

uranium hexafluoride in atmosphere.

UF6 Absorption Bands in mid IR

0 500 1000 1500 20001E-4

1E-3

0.01

0.1

1

10

100

10000.00 0.05 0.10 0.15 0.20

ν, cm-1

!!!

E, eV

Figure presents absorption cross section of UF6 molecule in mid IR. Perspective absorption bands for enrichment measurement and trace uranium hexafluoride detection are marked by red arrows.

Assignment ν, cm-1 σ, cm-1/atm Applicationv1+v3 1291 0.72 Enrichment measurement

v1+v4 853 0.12 Enrichment measurement

v3 625 350 Trace detection

Absorption bands identification

Combination band ν1+ ν3 was chosen for present experiment. Two other bands can be considered as alternative for UF6 enrichment

measurements and trace detection

800 900 1000 1100 1200 1300 14000

1Impurity

ν1+ν3

ν1+ν4

ν3+ν5

A

ν, cm-1

Experiment Ref. 2

Assignment ν, cm-1 σ, cm-1/atm2v3+v6 1386±2 0.0018

v1+v2+v6 1341 0.0088v1+v3 1290.9±0.5 0.72

2v2+v6 1211±2 0.0007v2+v3 1156.9±0.5 0.82

v3+2v6 905±2 0.0035v1+v4 852.8±0.5 0.12v3+v5 821 0.33

v3 625 350

Absorption spectrum of gas mixture under investigation and observed spectral features identification.

Isotope shifts for several UF6 normal vibration modes.

Isotope shifts,cm-1 235UF6-238UF6

ν1 0ν3 0.65±0.09ν4 0.16±0.09

Instrument Block Scheme

DL

PD3 PD2

PD1

1

2 3

PC

DL – diode laser; PD – photo detectors;PC – personal computer

Analytical channel with cell (1) containing gas under investigation. Reference channels with cell (2) containing methane and acetylene, and with Fabry-Perot etalon (3) were used to determine laser frequency tuning.

Instrument view Set up used to measure uranium hexafluoride enrichment

1 2

3

4

1 – diode laser in cryostat; 2 – analytical and reference channel with optical cells; 3 – photodetectors with preamplifiers in cryostat; 4 – electronic module with personal computer.

Instrument operation mode

0 500 1000 1500 2000

0.0

0.1

0.2

0.3

0.4

Sig

nal,

V

t, mks

Channel 1 Channel 2 Channel 3

Diode laser was excited by trapezium current pulse provided DL frequency tuning. Signals from photodiodes in three instrument channels were recorded simultaneously. Signals from channels 2 (methane absorption) and 3 (Fabry-Perot etalon interference fringes) were used to determine DL frequency tuning curve. Final accuracy of tuning curve determination was found to be better than 2 10-4 cm-1.

Positions of reference gas lines in channel 2 signal were used as feedback signal in DL frequency tuning stabilization mode. Using signal from channel 1 UF6 absorption in sample cell was determined.

Software development

Users interface of software developed to measure UF6 isotope ratio.

Software was written using LabView. Software developed controlled all instruments options, recorded signals, performed data processing, and stored results obtained on hard disk.

Diode Laser Spectroscopy of UF6

1291 1292 12930.4

0.5

0.6

0.7

σ, c

m-1/a

tm

ν, cm-1

Spectra were recorded using TDL based instrument developed. Fragment of experimental absorption cross section spectrum (blue points) and model spectra for 238UF6 (black line) and 235UF6 (red line).

Problem #2: Fine structure of UF6 spectra was not included in the present model. Accurate

spectrum of 235UF6 has to be measured.

Instrument Test at IAEA UF6 Loop in Seibersdorf

Several UF6 samples with calibrated enrichment were used. Figure shows results obtained for two calibrated samples: natural and high enriched ones. Sample cell was filled with calibrated gas and measurement procedure started. Fig.A presents measured partial pressure, Fig.B shows enrichment.

Accuracy in present case was limited by low quality diode laser and photo-diodes in use

0 200 400 60070

72

74

76

78

80

0 200 400 600

0

2

4

6

8

10

12

14

16

UF6

14.7%enrichmentU

F 6 p

ress

ure,

Tor

r

A

Isot

ope

ratio

235 U

F 6/237 U

F 6, %

Time, (arb. un)

UF6

0.7%enrichment

B

UF6 in Atmosphere

The necessity of detection of trace HF concentrations may arise in order to check the leaks of UF6 from the containers or technological processes, as well as to reveal the illegal activity in the manufacturing of 235-isotope enriched uranium. When getting to the air, it reacts with atmospheric water to yield the HF:

UF6 + 2H2O => UF2O2 (solid) + 4HF

HF is a volatile compound and can be detected with high sensitivity by diode laser based device. In this method the trace gas concentration is measured by scanning laser frequency over chosen molecular absorption line.

Block Scheme of Experimental Setup

DL – diode lasers; PD – photo detectors; PA – preamplifiers; PC – personal computer

Block scheme of experimental setup developed for investigation of uranium hexafluoride behavior in atmosphere.

IN-OUT Interface 1

Chamber

PD PA

PA

Fire Ware 1394

PD

PDPA

PCI

PD PA

DL 2

DL 1

Pumping out

PC

Notebook

Pumping in

IN-OUT Interface 2

Near IR – HF

Mid IR – UF6

Experimental Setup View

Diode Lasers

Near IR – HF

Mid IR – UF6

Chamber Photo Diodes

Computers

Simultaneous measurement of UF6 (left) and HF (right) concentration

The PC was time synchronized during uranium hexafluoride hydrolyze experiment. Data concentration of UF6 and HF was wrote in data files to PC.

Preliminary Results

16:28 16:29 16:30 16:31 16:32 16:33

0

1

2

3

4

5

P, T

orr

Time

UF6

HF

Ventilation on

Preliminary result of simultaneous measurement of trace UF6 and HF concentration using experimental setup described.

Resume: Local as well as remote monitoring of trace concentration of both UF6 and HF

trace concentrations can be performed using TDLS.

TDL based instrument modifications

TDL based instrument for local measurements of trace molecule concentration

TDL based instrument for remote monitoring


Recommended