Abstract:The thermal atomic layer etching (ALE) of WO and W was demonstrated with new "conversion-fluorination" and "oxidation-conversion-fluorination" etching mechanisms. Both of these mechanisms are based on sequential, self-limiting reactions. WO ALE was achieved by a "conversion-fluorination" mechanism using an AB exposure sequence with boron trichloride (BCl) and hydrogen fluoride (HF). BCl converts the WO surface to a BO layer while forming volatile WOCl products. Subsequently, HF spontaneously etches the BO laye… Show more
“…For the oxygen ion beam, 300 W of RF power was applied to the ICP source at 1 mTorr of O 2 while applying + 30– + 100 V to the first grid, −100 V to the second grid, and 0 V (grounded) to the third grid. The formation of WO x was estimated by the increased W thickness after the oxygen ion beam exposure using a surface profilometer because, during the oxygen exposure, the thickness of W is increased by the formation of WO x . (In fact, because it is difficult to measure the thickness of a self‐limiting oxidation step of a few angstroms with a profilometer, the oxidation time was increased until the oxide thickness can be measured by the profilometer and the data were extrapolated to the lower oxidation time.)…”
Section: Resultsmentioning
confidence: 99%
“…The formation of WO x was estimated by the increased W thickness after the oxygen ion beam exposure using a surface profilometer because, during the oxygen exposure, the thickness of W is increased by the formation of WO x . [33] (In fact, because it is difficult to measure the thickness of a self-limiting oxidation step of a few angstroms with a profilometer, the oxidation time was increased until the oxide thickness can be measured by the profilometer and the data were extrapolated to the lower oxidation time.) Figure 2(b) shows the changes in WO x thickness on the W surface measured by the surface profilometer with increasing first grid voltage from + 30 to + 100 V and O x + ion exposure time from 0 to 60 s. The first grid voltage is directly related to the oxygen ion energy from the ion source and the ion energy distributions measured by a retarding grid ion energy analyzer for the different first grid voltages are shown in Figure S1.…”
Section: Resultsmentioning
confidence: 99%
“…For the application of W to next generation device interconnection, ALE technology of W is known to be required . For the W ALE method, a W thermal ALE obtained through an oxidation‐conversion‐fluorination etch mechanism, which is a three step ALE composed of oxidation using O 3 , the conversion to a volatile oxychloride compound using BCl 3 , and the final removal of the surface reside compound by fluorination by HF, is reported . In addition, a thermal ALE of W using sequential exposure to O 2 (or O 3 ) and WF 6 , where, W is oxidized using O 2 or O 3 to form WO 3 (s), and the WO 3 is removed by forming volatile WO 2 F 2 (g) by the reaction with HF has been investigated .…”
Section: Introductionmentioning
confidence: 99%
“…[31,32] For the W ALE method, a W thermal ALE obtained through an oxidation-conversion-fluorination etch mechanism, which is a three step ALE composed of oxidation using O 3 , the conversion to a volatile oxychloride compound using BCl 3 , and the final removal of the surface reside compound by fluorination by HF, is reported. [33] In addition, a thermal ALE of W using sequential exposure to O 2 (or O 3 ) and WF 6 , where, W is oxidized using O 2 or O 3 to form WO 3 (s), and the WO 3 is removed by forming volatile WO 2 F 2 (g) by the reaction with HF has been investigated. [34] Even though, selflimited precise etching of W with the rates of a few Å/ cycle could be obtained with the ALE methods investigated until now, all of these methods are isotropic W ALE methods and an anisotropic W ALE method which can form anisotropic etch profiles of W has not been investigated yet.…”
Atomic layer etching (ALE) has advantages such as precise thickness control, high etch selectivity, and no‐increase in surface roughness which can be applied to sub 10 nm semiconductor device fabrication. In this study, anisotropic ALE of tungsten (W), which is used as an interconnect layer and gate material of semiconductor devices, was investigated by sequentially exposing to F radicals by NF3 plasma to form a WFy layer and following exposure to an oxygen ion beam to remove the WFy layer by forming volatile WOxFy at room temperature. A wide ALE window of F radical adsorption time of ( ≥ 10 s/cycle) and Ox+ ion desorption time of (10 ≤ t ≤ 50 s/cycle at + 44–51 eV of Ox+ ion energy) could be identified, and at the ALE conditions, a precise etch rate of ~2.6 Å/cycle was obtained while increasing the W etch depth linearly with increasing the number of etch cycles. At the optimized W ALE conditions, the W surface roughness after the W ALE was similar to the as‐received W and the etch selectivity over SiO2 was close to infinite. However, after the W ALE, ~ 10% F diffused into W was observed on the etched W surface, and which could be removed by a following process.
“…For the oxygen ion beam, 300 W of RF power was applied to the ICP source at 1 mTorr of O 2 while applying + 30– + 100 V to the first grid, −100 V to the second grid, and 0 V (grounded) to the third grid. The formation of WO x was estimated by the increased W thickness after the oxygen ion beam exposure using a surface profilometer because, during the oxygen exposure, the thickness of W is increased by the formation of WO x . (In fact, because it is difficult to measure the thickness of a self‐limiting oxidation step of a few angstroms with a profilometer, the oxidation time was increased until the oxide thickness can be measured by the profilometer and the data were extrapolated to the lower oxidation time.)…”
Section: Resultsmentioning
confidence: 99%
“…The formation of WO x was estimated by the increased W thickness after the oxygen ion beam exposure using a surface profilometer because, during the oxygen exposure, the thickness of W is increased by the formation of WO x . [33] (In fact, because it is difficult to measure the thickness of a self-limiting oxidation step of a few angstroms with a profilometer, the oxidation time was increased until the oxide thickness can be measured by the profilometer and the data were extrapolated to the lower oxidation time.) Figure 2(b) shows the changes in WO x thickness on the W surface measured by the surface profilometer with increasing first grid voltage from + 30 to + 100 V and O x + ion exposure time from 0 to 60 s. The first grid voltage is directly related to the oxygen ion energy from the ion source and the ion energy distributions measured by a retarding grid ion energy analyzer for the different first grid voltages are shown in Figure S1.…”
Section: Resultsmentioning
confidence: 99%
“…For the application of W to next generation device interconnection, ALE technology of W is known to be required . For the W ALE method, a W thermal ALE obtained through an oxidation‐conversion‐fluorination etch mechanism, which is a three step ALE composed of oxidation using O 3 , the conversion to a volatile oxychloride compound using BCl 3 , and the final removal of the surface reside compound by fluorination by HF, is reported . In addition, a thermal ALE of W using sequential exposure to O 2 (or O 3 ) and WF 6 , where, W is oxidized using O 2 or O 3 to form WO 3 (s), and the WO 3 is removed by forming volatile WO 2 F 2 (g) by the reaction with HF has been investigated .…”
Section: Introductionmentioning
confidence: 99%
“…[31,32] For the W ALE method, a W thermal ALE obtained through an oxidation-conversion-fluorination etch mechanism, which is a three step ALE composed of oxidation using O 3 , the conversion to a volatile oxychloride compound using BCl 3 , and the final removal of the surface reside compound by fluorination by HF, is reported. [33] In addition, a thermal ALE of W using sequential exposure to O 2 (or O 3 ) and WF 6 , where, W is oxidized using O 2 or O 3 to form WO 3 (s), and the WO 3 is removed by forming volatile WO 2 F 2 (g) by the reaction with HF has been investigated. [34] Even though, selflimited precise etching of W with the rates of a few Å/ cycle could be obtained with the ALE methods investigated until now, all of these methods are isotropic W ALE methods and an anisotropic W ALE method which can form anisotropic etch profiles of W has not been investigated yet.…”
Atomic layer etching (ALE) has advantages such as precise thickness control, high etch selectivity, and no‐increase in surface roughness which can be applied to sub 10 nm semiconductor device fabrication. In this study, anisotropic ALE of tungsten (W), which is used as an interconnect layer and gate material of semiconductor devices, was investigated by sequentially exposing to F radicals by NF3 plasma to form a WFy layer and following exposure to an oxygen ion beam to remove the WFy layer by forming volatile WOxFy at room temperature. A wide ALE window of F radical adsorption time of ( ≥ 10 s/cycle) and Ox+ ion desorption time of (10 ≤ t ≤ 50 s/cycle at + 44–51 eV of Ox+ ion energy) could be identified, and at the ALE conditions, a precise etch rate of ~2.6 Å/cycle was obtained while increasing the W etch depth linearly with increasing the number of etch cycles. At the optimized W ALE conditions, the W surface roughness after the W ALE was similar to the as‐received W and the etch selectivity over SiO2 was close to infinite. However, after the W ALE, ~ 10% F diffused into W was observed on the etched W surface, and which could be removed by a following process.
“…Indeed, progress toward the isotropic thermal ALE of metallic W has been reported by the groups of George and Parsons. The work reported by George et al ( 13 ) has shown the quasi-ALE of metallic W via a conversion etch mechanism utilizing ozone (O 3 ), BCl 3 , and anhydrous HF vapor. In this system, ozone was used to oxidize the W surface to WO 3 in a diffusion-limited process, which then reacts with BCl 3 to generate a volatile etch product in the form of WO x Cl y while tandemly generating a B 2 O 3 surface layer, which is then susceptible to self-limiting etch by HF.…”
Thermal
atomic layer etch (ALE) of W metal can be achieved by sequential
self-limiting oxidation and chlorination reactions at elevated temperatures.
In this paper, we analyze the reaction mechanisms of W ALE using the
first-principles simulation. We show that oxidizing agents such as
O
2
, O
3
, and N
2
O can be used to produce
a WO
x
surface layer in the first step
of an ALE process with ozone being the most reactive. While the oxidation
pulse on clean W is very exergonic, our study suggests that runaway
oxidation of W is not thermodynamically favorable. In the second ALE
pulse, WCl
6
and Cl
2
remove the oxidized surface
W atoms by the formation of volatile tungsten oxychloride (W
x
O
y
Cl
z
) species. In this pulse, each adsorbed WCl
6
molecule was found to remove one surface W atom with a moderate
energy cost. Our calculations further show that the desorption of
the additional etch products is endothermic by up to 4.7 eV. Our findings
are consistent with the high temperatures needed to produce ALE in
experiments. In total, our quantum chemical calculations have identified
the lowest energy pathways for ALE of tungsten metal along with the
most likely etch products, and these findings may help guide the development
of improved etch reagents.
Plasma etching or reactive ion etching (RIE) has been the workhorse for patterning of semiconductor devices since the early 1980s when it replaced wet etching in manufacturing. Today, RIE is reaching levels of performance that were unimaginable back then. At the same time, etching technologies such as atomic layer etching (ALE), radical dry vapor etching, and ion beam etching are finding their way into manufacturing for certain applications.
Herein, we present an overview of dry etching technologies used in semiconductor manufacturing. The emphasis is on the elementary surface processes and how they impact the performance on the wafer. We will start from less complex etching technologies, which use just one kind of etching species, such as neutrals, radicals, or ions. Then we combine these techniques into cycling processes, which leads to the discussion of ALE. The highest level of complexity is reached in RIE with simultaneous species fluxes. Reactor designs for the various etching technologies and process control will be covered. Finally, the outlook into the future of semiconductor device etching will be given.
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