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Development of Atomic Layer Etching (ALEt) for GaN-based materials
Congying You, C. Mannequin, G. Jacopin, T. Chevolleau, C. Durand, C. Vallee, H. Mariette, M. Sasaki, E. Gheeraert
To cite this version:
Congying You, C. Mannequin, G. Jacopin, T. Chevolleau, C. Durand, et al.. Development of Atomic Layer Etching (ALEt) for GaN-based materials. International Workshop on Nitride Semiconductors, Nov 2018, Kanazawa, Japan. �hal-02008012�
Development of Atomic Layer Etching (ALEt) for GaN-based materials
Congying You
1,2*
, C. Mannequin
1
, G. Jacopin
2
, T. Chevolleau
3
, C. Durand
4
, C. Vallée
1,3
, H. Mariette
1,2
,
M. Sasaki
1
, E. Gheeraert
1,2
*E-mail: congying.you@neel.cnrs.fr
1University of Tsukuba, Tsukuba 305-8573, Japan,
2
Univ. Grenoble-Alpes, Institut Néel, 25 Avenue des Martyrs, Grenoble 38000, France,
3Univ. Grenoble-Alpes, LTM, Grenoble 38000, France,
4
Univ. Grenoble-Alpes, INAC/PHELIQS, 18 Avenue des Martyrs, Grenoble 38000, France
1. What is Atomic Layer Etching (ALEt)?
1
Advantages:
• Fast and deep etching
• Separate controlled of Plasma density (neutrals, radicals, ions), Ionic Fluxes and Ions Energies
Advantages:
- Separation:
Chemistry (precursor)/ionic bombardment (co-reactant)
- Etch rate controlled by Numb. of cycles
- Different plasma (or gases): for chemistry and ionic bombardment
Challenges:
- Keep the “self-limiting” feature - Slow:
Etch profile defined by Numb. of cycles (< 1nm/cycle) - Monitoring of etched thickness
Limitations:
• Simultaneous effect of chemistry and ionic bombardment • Difficult to control Surface States (morphology and
composition)
Atomic Layer Etching
2. Experimental procedures
sapphire GaN (3 μm) SiO2 (450nm) sapphire GaN (3 μm) SiO2 coating SQW sample SiO2 patterning SiO2 sapphire GaN (3 μm) ALEt 200 cycles SiO2 sapphire GaN (3 μm) SiO2 sapphire GaN After-etch Characterization sapphire GaN (3 μm) sapphire GaN (3 μm) Photoresist (1400nm) sapphire GaN (3 μm) PR PR ALEt 200 cycles sapphire GaN (3 μm) PR PR sapphire GaN After-etch Characterization Photoresist (PR) coating PR patterningCapping layer: GaN (5 nm ) Single quantum well: InGaN
with 18% In (2.75 nm; 750°C ) GaN (20 nm; 850°C) Underlayer: InGaN with 3-5% In (50 nm; 750°C) sapphire GaN (3 μm)
Thomas Swan (AIXTRON) MOCVD
Development of ALEt on SAMCO ICP-RIE 200 iP
Deposition:
GaN layers with embedded
InGaN Single Quantum
Well (SQW)
Holes fabrication process and Experimental procedures:
1- Planar GaN layer
2- Planar InGaN SQW layer
PR removed sapphire
GaN
SAMCO ICP-RIE 200iP
+
ICP-Coil
RF-Source
(Wsource)
Polarization
RF-Bias
(Wbias)
Plasma Neutrals,Radicals IonsIons
Energies:
V
plasma– V
DC(Wbias)
Plasma density:
Neutrals, Radicals
Ions
(Wsource)
+
Other
Parameters:
Gas comp.
Pressure
Exposition
time
Our ALE process (to be patented):
Total repetition: 200 ALEt cycles
pur
ge
Cl
2time
1st cycle 2nd cycle 3rd cycleAdsorption
pur
ge
Activation
Cl2-based gas mixture (Mad) Exposure time tad Wsource No Wbias Gas mixture (Mac) Exposure time tac Wsource Wbias
4. Comparison of in- and out-of ALEt window etched samples
3. ALEt Etch rate as a function of Activation Bias
etched SQW samples with gas X: ICP/Bias 100/25W (Vdc=19V) (top) and ICP/Bias 100/45W (Vdc=32V) (down) and death layer on the etch edge
Cathodo-Luminescence of SQW samples : Estimation of deadlayer thickness
SEM SQW CL signalT=300K SQW CL signal T=300K SEM 400nm 1um
Effect of Wbias on ALE etching rate
and
( Self-bias voltage and ion energy)
0 0,5 1 1,5 2 2,5 3 0 5 10 15 20 25 30 35 40 e tc h r ate/cycl e (nm) Vdc(V) 1 monolayer/cycle 2 monolayers/cycle
Etch rate in function of the self-bias voltage
0 0,5 1 1,5 2 2,5 0 5 10 15 20 25 30 35 40 Et ch r ate/cycl e (nm) Vdc (V)
Etch Rate in function of the self-bias voltage
1 monolayer/cycle 2 monolayers/cycle
Argon Gas X
Atomic Layer Etching window
Optimization of the Activation step:
The best Etch rate: near 2 monolayers/ cycle
Gas X have a better control of ALEt
RMS=68pm
RMS=177pm RMS=428pm
For undoped-GaN
and GaN + embedded SQW GaN
200 ALE cycles
Etching rate = etched thickness (SEM)/200
Contrast SEM: 370nm (tilted edge) Dead layer(CL 425nm slope): 900nm
pur
ge
Cl
2time
1st cycleAdsorption
pur
ge
Activation
Cl2-based gas mixture (Mad) Exposure time tad Wsource No Wbias Gas mixture (Mac) Exposure time tac Wsource Wbias
M
ac= Ar
M
ac= X
SiO2-masked samples In-window quasi-ALEt Out-of-window cyclic etching
Contrast SEM: 175nm (sharp edge) Dead layer(CL 425nm slope): 400nm In-window quasi-ALEt
Out-of-window cyclic etching
6. Conclusions and perspectives
tad - tp - tac+15 - tp
ER about 0.74
t
ad+1 - t
p- t
ac- t
pER 0.59nm/cycle
Activation step
Not fully self-limiting Need to improve
Adsorption step self-limiting verified
longer adsorption time
longer activation time
tad+2 - tp - tac – tp
ER 0.57nm/cycle
Optimizations real ALEt +limiting the dead layer
Improve the Activation step (take a Bias on the ALEt windowchange the ICP power);
change pressure in different steps, etc
verify other advanced properties Apply to Electronic/optoelectronic device
5.Demonstration of the self-limiting
1. Gas X has a better etch control on the ALEt process
2. Quasi ALEt has a better etch quality: sharp border; thinner dead layer
t
ad- t
purge(t
p)- t
ac- t
pER 0.58nm/cycle
tad - tp - tac+5 - tp
ER 0.59nm/cycle Base point (gas X in-window sample)