CobaltMaghrebV1, PascalFrancis, Curation, bibRecord, 000237

Role of the active layer thickness on the sensitivity of WO3 gas sensors

Identifieur interne : 000237 ( PascalFrancis/Curation ); précédent : 000236; suivant : 000238

Role of the active layer thickness on the sensitivity of WO3 gas sensors

Auteurs : K. Aguir [France] ; J. Guerin [France] ; N. Mliki [Tunisie] ; M. Bendahan [France]

Source :

International journal of nanotechnology [ 1475-7435 ] ; 2012.

RBID : Pascal:12-0133012

Descripteurs français

Pascal (Inist)
- Couche active, Epaisseur couche, Capteur de gaz, Matériau capteur, Couche épaisse, Addition béryllium, Couche superficielle, Cobalt, Effet dimensionnel, Sélectivité, Modélisation, Etude théorique, Polycristal, Semiconducteur, Couche mince, Nanomatériau, WO3, SnO2, CuO, ZnO, Substrat cobalt, 0707D, 8107B.
Wicri :
- topic : Cobalt.

English descriptors

KwdEn :
- Active layer, Beryllium additions, Cobalt, Gas sensors, Layer thickness, Modelling, Nanostructured materials, Polycrystals, Selectivity, Semiconductor materials, Sensor materials, Size effect, Surface layers, Theoretical study, Thick films, Thin films.

Abstract

Sensitive materials in gas sensors are often polycrystalline semiconducting oxides such as WO₃, SnO₂, CuO or ZnO. They are most often composed of nanometric grains. They can be deposited either as thin or thick films. The film thickness plays an important role in the response stability and sensitivity of sensors. It is now well accepted that the relationship between the surface and volume of the sensitive layer plays a major role in the efficiency of detection. Many experimental and theoretical works were reported in explaining the experimental sensitivity vs. thickness relationships reported for the gas sensors prepared by different fabrication techniques. In addition, significant changes can be expected by adding catalytic nanograins in small quantities on the surface of the sensitive layers. For example, cobalt nanograins deposited on the surface of WO₃ sensors produce an important change in the WO₃ conductance. Indeed, cobalt changes the conduction type of the sensors from n- to p-type. This paper describes the effect of reducing the size of the sensors and nanostructured sensitive materials on the sensor response.

A01	`01`	`1`		`@0 1475-7435`
A03		`1`		`@0 Int. j. nanotechnol.`
A05				`@2 9`
A06				`@2 3-7`
A08	`01`	`1`	`ENG`	`@1 Role of the active layer thickness on the sensitivity of WO₃ gas sensors`
A09	`01`	`1`	`ENG`	`@1 On Nanotechnology in France III: C'Nano PACA`
A11	`01`	`1`		`@1 AGUIR (K.)`
A11	`02`	`1`		`@1 GUERIN (J.)`
A11	`03`	`1`		`@1 MLIKI (N.)`
A11	`04`	`1`		`@1 BENDAHAN (M.)`
A12	`01`	`1`		`@1 HANBÜCHEN (Margrit) @9 ed.`
A12	`02`	`1`		`@1 LANNOO (Michel) @9 ed.`
A12	`03`	`1`		`@1 BLANC (Wilfried) @9 ed.`
A12	`04`	`1`		`@1 DJENIZIAN (Thierry) @9 ed.`
A12	`05`	`1`		`@1 SANTINACCI (Lionel) @9 ed.`
A14	`01`			`@1 IM2NP, CNRS 6242, Aix-Marseille University, FST, S152 @2 13397 Marseille @3 FRA @Z 1 aut. @Z 2 aut.`
A14	`02`			`@1 LMOP, Faculty of Sciences, Tunis El Manar University @2 Tunis @3 TUN @Z 3 aut.`
A14	`03`			`@1 IM2NP, CNRS 6242, Aix-Marseille University, FST, S152 @2 13397 Marseille @3 FRA @Z 4 aut.`
A15	`01`			`@1 C'Nano PACA, Campus Luminy - Case 913 @2 13288 Marseille @3 FRA @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut.`
A20				`@1 471-479`
A21				`@1 2012`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 27530 @5 354000508430030190`
A44				`@0 0000 @1 © 2012 INIST-CNRS. All rights reserved.`
A45				`@0 23 ref.`
A47	`01`	`1`		`@0 12-0133012`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 International journal of nanotechnology`
A66	`01`			`@0 CHE`
C01	`01`		`ENG`	@0 Sensitive materials in gas sensors are often polycrystalline semiconducting oxides such as WO₃, SnO₂, CuO or ZnO. They are most often composed of nanometric grains. They can be deposited either as thin or thick films. The film thickness plays an important role in the response stability and sensitivity of sensors. It is now well accepted that the relationship between the surface and volume of the sensitive layer plays a major role in the efficiency of detection. Many experimental and theoretical works were reported in explaining the experimental sensitivity vs. thickness relationships reported for the gas sensors prepared by different fabrication techniques. In addition, significant changes can be expected by adding catalytic nanograins in small quantities on the surface of the sensitive layers. For example, cobalt nanograins deposited on the surface of WO₃ sensors produce an important change in the WO₃ conductance. Indeed, cobalt changes the conduction type of the sensors from n- to p-type. This paper describes the effect of reducing the size of the sensors and nanostructured sensitive materials on the sensor response.
C02	`01`	`3`		`@0 001B80A07B`
C02	`02`	`3`		`@0 001B00G07D`
C03	`01`	`X`	`FRE`	`@0 Couche active @5 01`
C03	`01`	`X`	`ENG`	`@0 Active layer @5 01`
C03	`01`	`X`	`SPA`	`@0 Capa activa @5 01`
C03	`02`	`X`	`FRE`	`@0 Epaisseur couche @5 02`
C03	`02`	`X`	`ENG`	`@0 Layer thickness @5 02`
C03	`02`	`X`	`SPA`	`@0 Espesor capa @5 02`
C03	`03`	`3`	`FRE`	`@0 Capteur de gaz @5 03`
C03	`03`	`3`	`ENG`	`@0 Gas sensors @5 03`
C03	`04`	`3`	`FRE`	`@0 Matériau capteur @5 04`
C03	`04`	`3`	`ENG`	`@0 Sensor materials @5 04`
C03	`05`	`3`	`FRE`	`@0 Couche épaisse @5 05`
C03	`05`	`3`	`ENG`	`@0 Thick films @5 05`
C03	`06`	`3`	`FRE`	`@0 Addition béryllium @5 06`
C03	`06`	`3`	`ENG`	`@0 Beryllium additions @5 06`
C03	`07`	`3`	`FRE`	`@0 Couche superficielle @5 07`
C03	`07`	`3`	`ENG`	`@0 Surface layers @5 07`
C03	`08`	`3`	`FRE`	`@0 Cobalt @2 NC @5 08`
C03	`08`	`3`	`ENG`	`@0 Cobalt @2 NC @5 08`
C03	`09`	`3`	`FRE`	`@0 Effet dimensionnel @5 09`
C03	`09`	`3`	`ENG`	`@0 Size effect @5 09`
C03	`10`	`X`	`FRE`	`@0 Sélectivité @5 10`
C03	`10`	`X`	`ENG`	`@0 Selectivity @5 10`
C03	`10`	`X`	`SPA`	`@0 Selectividad @5 10`
C03	`11`	`3`	`FRE`	`@0 Modélisation @5 11`
C03	`11`	`3`	`ENG`	`@0 Modelling @5 11`
C03	`12`	`3`	`FRE`	`@0 Etude théorique @5 12`
C03	`12`	`3`	`ENG`	`@0 Theoretical study @5 12`
C03	`13`	`3`	`FRE`	`@0 Polycristal @5 15`
C03	`13`	`3`	`ENG`	`@0 Polycrystals @5 15`
C03	`14`	`3`	`FRE`	`@0 Semiconducteur @5 16`
C03	`14`	`3`	`ENG`	`@0 Semiconductor materials @5 16`
C03	`15`	`3`	`FRE`	`@0 Couche mince @5 17`
C03	`15`	`3`	`ENG`	`@0 Thin films @5 17`
C03	`16`	`3`	`FRE`	`@0 Nanomatériau @5 18`
C03	`16`	`3`	`ENG`	`@0 Nanostructured materials @5 18`
C03	`17`	`3`	`FRE`	`@0 WO3 @4 INC @5 46`
C03	`18`	`3`	`FRE`	`@0 SnO2 @4 INC @5 47`
C03	`19`	`3`	`FRE`	`@0 CuO @4 INC @5 48`
C03	`20`	`3`	`FRE`	`@0 ZnO @4 INC @5 49`
C03	`21`	`3`	`FRE`	`@0 Substrat cobalt @4 INC @5 50`
C03	`22`	`3`	`FRE`	`@0 0707D @4 INC @5 65`
C03	`23`	`3`	`FRE`	`@0 8107B @4 INC @5 71`
N21				`@1 100`

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Le document en format XML

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<term>Modelling</term>
<term>Nanostructured materials</term>
<term>Polycrystals</term>
<term>Selectivity</term>
<term>Semiconductor materials</term>
<term>Sensor materials</term>
<term>Size effect</term>
<term>Surface layers</term>
<term>Theoretical study</term>
<term>Thick films</term>
<term>Thin films</term>
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<keywords scheme="Pascal" xml:lang="fr"><term>Couche active</term>
<term>Epaisseur couche</term>
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<term>Matériau capteur</term>
<term>Couche épaisse</term>
<term>Addition béryllium</term>
<term>Couche superficielle</term>
<term>Cobalt</term>
<term>Effet dimensionnel</term>
<term>Sélectivité</term>
<term>Modélisation</term>
<term>Etude théorique</term>
<term>Polycristal</term>
<term>Semiconducteur</term>
<term>Couche mince</term>
<term>Nanomatériau</term>
<term>WO3</term>
<term>SnO2</term>
<term>CuO</term>
<term>ZnO</term>
<term>Substrat cobalt</term>
<term>0707D</term>
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<front><div type="abstract" xml:lang="en">Sensitive materials in gas sensors are often polycrystalline semiconducting oxides such as WO<sub>3</sub>
, SnO<sub>2</sub>
, CuO or ZnO. They are most often composed of nanometric grains. They can be deposited either as thin or thick films. The film thickness plays an important role in the response stability and sensitivity of sensors. It is now well accepted that the relationship between the surface and volume of the sensitive layer plays a major role in the efficiency of detection. Many experimental and theoretical works were reported in explaining the experimental sensitivity vs. thickness relationships reported for the gas sensors prepared by different fabrication techniques. In addition, significant changes can be expected by adding catalytic nanograins in small quantities on the surface of the sensitive layers. For example, cobalt nanograins deposited on the surface of WO<sub>3</sub>
 sensors produce an important change in the WO<sub>3</sub>
 conductance. Indeed, cobalt changes the conduction type of the sensors from n- to p-type. This paper describes the effect of reducing the size of the sensors and nanostructured sensitive materials on the sensor response.</div>
</front>
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 gas sensors</s1>
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<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
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<fA14 i1="02"><s1>LMOP, Faculty of Sciences, Tunis El Manar University</s1>
<s2>Tunis</s2>
<s3>TUN</s3>
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<sZ>4 aut.</sZ>
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<s1>© 2012 INIST-CNRS. All rights reserved.</s1>
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<fA60><s1>P</s1>
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</fA66>
<fC01 i1="01" l="ENG"><s0>Sensitive materials in gas sensors are often polycrystalline semiconducting oxides such as WO<sub>3</sub>
, SnO<sub>2</sub>
, CuO or ZnO. They are most often composed of nanometric grains. They can be deposited either as thin or thick films. The film thickness plays an important role in the response stability and sensitivity of sensors. It is now well accepted that the relationship between the surface and volume of the sensitive layer plays a major role in the efficiency of detection. Many experimental and theoretical works were reported in explaining the experimental sensitivity vs. thickness relationships reported for the gas sensors prepared by different fabrication techniques. In addition, significant changes can be expected by adding catalytic nanograins in small quantities on the surface of the sensitive layers. For example, cobalt nanograins deposited on the surface of WO<sub>3</sub>
 sensors produce an important change in the WO<sub>3</sub>
 conductance. Indeed, cobalt changes the conduction type of the sensors from n- to p-type. This paper describes the effect of reducing the size of the sensors and nanostructured sensitive materials on the sensor response.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B80A07B</s0>
</fC02>
<fC02 i1="02" i2="3"><s0>001B00G07D</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE"><s0>Couche active</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="X" l="ENG"><s0>Active layer</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="X" l="SPA"><s0>Capa activa</s0>
<s5>01</s5>
</fC03>
<fC03 i1="02" i2="X" l="FRE"><s0>Epaisseur couche</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="X" l="ENG"><s0>Layer thickness</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="X" l="SPA"><s0>Espesor capa</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Capteur de gaz</s0>
<s5>03</s5>
</fC03>
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<s5>03</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Matériau capteur</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Sensor materials</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Couche épaisse</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Thick films</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Addition béryllium</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Beryllium additions</s0>
<s5>06</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Couche superficielle</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Surface layers</s0>
<s5>07</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Cobalt</s0>
<s2>NC</s2>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Cobalt</s0>
<s2>NC</s2>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Effet dimensionnel</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Size effect</s0>
<s5>09</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Sélectivité</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Selectivity</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Selectividad</s0>
<s5>10</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Modélisation</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Modelling</s0>
<s5>11</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Etude théorique</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Theoretical study</s0>
<s5>12</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Polycristal</s0>
<s5>15</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Polycrystals</s0>
<s5>15</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Semiconducteur</s0>
<s5>16</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Semiconductor materials</s0>
<s5>16</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Couche mince</s0>
<s5>17</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Thin films</s0>
<s5>17</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Nanomatériau</s0>
<s5>18</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG"><s0>Nanostructured materials</s0>
<s5>18</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>WO3</s0>
<s4>INC</s4>
<s5>46</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>SnO2</s0>
<s4>INC</s4>
<s5>47</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>CuO</s0>
<s4>INC</s4>
<s5>48</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>ZnO</s0>
<s4>INC</s4>
<s5>49</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE"><s0>Substrat cobalt</s0>
<s4>INC</s4>
<s5>50</s5>
</fC03>
<fC03 i1="22" i2="3" l="FRE"><s0>0707D</s0>
<s4>INC</s4>
<s5>65</s5>
</fC03>
<fC03 i1="23" i2="3" l="FRE"><s0>8107B</s0>
<s4>INC</s4>
<s5>71</s5>
</fC03>
<fN21><s1>100</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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	Serveur d'exploration sur le cobalt au Maghreb
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Serveur d'exploration sur le cobalt au Maghreb

Role of the active layer thickness on the sensitivity of WO3 gas sensors

Role of the active layer thickness on the sensitivity of WO3 gas sensors

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