Characterizing
and abating ion implant process effluents
Josep
Arnó, Joseph Sweeney, Paul Marganski, and Brian Kingston, ATMI;
and Steven Roberge and M. Christopher Dolan, Axcelis Technologies
Ion
implant processes utilize materials that are potentially toxic to humans
and damaging to the environment. Conventional dopants include arsenic,
phosphorus, and boron, many precursors of which are delivered as gases
in their halogenated or hydrogenated forms. Arsine (AsH3),
phosphine (PH3), and boron trifluoride (BF3),
which are highly toxic (hydrides) and corrosive (halogens), are among
the most common of the precursor gases. Table I indicates the threshold
limit values (TLVs) and immediate-danger-to-life-and-health (IDLH) levels
of these gases.
In
order to ensure safe operations, many IC manufacturers use sub-atmospheric-pressure
gas-delivery sources and implement other measures to minimize personnel
exposure to implant dopants.
Only
small fractions of the dopants introduced into the tool are implanted
onto wafers. The bulk of the source materials are either deposited as
solids on the walls of the source and beam-line chambers or are exhausted
through various pumps. A typical ion implanter accommodates a number
of turbo pumps, backed by roughing pumps that evacuate chambers in a
continuous mode. In addition, cryogenic, or cryo, pumps collect condensable
materials, which are vented intermittently during cryoregeneration processes.
Ion
implantation tools present a unique emissions-abatement challenge: scrubbing
low flow rates of highly toxic materials that are diluted with relatively
high flow rates of nitrogen (N2) from the roughing
and cryo pumps. Four traditional abatement methods have the potential
to meet this challenge. Water scrubbers using injected chemical enhancers
can achieve the efficiency necessary to remove implant effluent materials.
However, such systems' cost of ownership and relatively large footprint,
as well as the need to dispose of arsenic-containing liquids, limit
their practical use. Thermal and plasma abatement methods simply dissociate
materials into solid form, thereby generating hazardous dust. In addition,
the electrical or other fuel costs of such tools can be prohibitive,
considering the relatively small volume of materials being vented from
implanters. Thus, of the four possible methods, dry scrubbers seem best
suited for this application.
|
Dopant
Name
|
TLV
Concentration Value (ppm) |
IDLH
Concentration Value (ppm) |
| Arsine
(AsH3) |
0.05
|
3
|
| Phosphine
(PH3) |
0.3
|
50
|
| Boron
trifluoride (BF3) |
1a
|
25
|
|
| Table I: Threshold limit values
and immediate-danger-to-life-and-health values of selected dopant
gases. |
Whichever
method is adopted, the optimal performance of the abatement control
equipment relies on a profound understanding of the fate of the materials
introduced into the tool as a function of time and type of pump. Few
studies have been published describing the nature and concentration
of gas-phase species emitted during ion implantation. One characterized
the process effluents of a high-current implanter during implantation
of AsH3, PH3, BF3, and silicon tetrafluoride
(SiF4) by measuring the concentration of gas-phase species
from roughing and cryo pumps using Fourier transform infrared (FTIR)
spectroscopic techniques.1 Another study, by other researchers,
used the same method to analyze the exhaust of the roughing pump of
a high-energy implanter during implantation of AsH3 and PH3.2
 |
| Figure 1: Schematic of the 200-mm
ion implanter's chambers and pumping system, including the dry scrubbers
installed on top of the tool. |
The
research project described in this article combined the comprehensive
characterization of gas-phase species at the exhaust of all roughing
and cryo pumps of a 200-mm implanter with the performance testing of
point-of-exhaust scrubbers installed after each pump. The gas-phase
analyses were performed at the Axcelis Technologies development laboratories
in Beverly, MA, during standard implant processes using AsH3,
PH3, and BF3 sources. Measurements were taken
with an FTIR spectrometer operating in a quantitative, continuous, in-line
mode.
The
efficiencies and pressure drops of the abatement tools were characterized
during test implantation runs using the three common dopant species
and during cryoregeneration. A comparison between inlet and outlet concentrations
provided information about the effectiveness of the scrubbers. Pressure-drop
and scrubbing efficiency also were examined periodically for one year
to validate long-term operation of the abatement technique. This work
describes gas-phase emissions only; it does not account for solid-phase
by-products.
Experimental
Setup and Equipment
For
this study, 40 X 20 roughing pumps from Ebara (Tokyo) were used. The
roughing and cryo pumps installed on an Axcelis high-energy 200-mm GSD-VHE
ion implanter were equipped with zero-footprint Novasafe dry scrubbers
from ATMI (Danbury, CT). Figure 1 is a schematic of the implanter chambers,
pumps, and scrubbers, and the photograph in Figure 2 shows three of
the small scrubbers installed on top of the implanter tool. Drawings
showing exterior and interior views of a scrubber are provided in Figure
3. Measuring 30 cm high and 25 cm in diameter, each scrubber is filled
with two layers of chemisorption media with the capacity to abate hydride
and acid implant dopants. Sampling ports installed at the inlet and
outlet of the scrubbers were used to collect gas streams into a Model
I2000 FTIR spectrometer from Midac (Irvine, CA) and a portable gas monitor,
respectively.
 |
| Figure 2: The ion implanter with
three scrubbers installed on top. |
The
spectrometer used to measure the implanter effluent gases at the scrubber
inlet included a multipass (10-m path length) gas cell to quantitatively
measure the concentrations of IR-active materials in situ in a continuous
mode. The instrument was calibrated against the implant dopants AsH3,
PH3, and BF3. Full-spectra
(from 600 to 4500 cm1) measurements were collected
periodically (every 416 seconds depending on the specific experiment)
at a 0.5-cm1 resolution. Samples were drawn continuously
at an approximately 4-std L/min flow rate using a Teflon diaphragm pump.
The
detection limits of the portable gas monitor used to analyze the scrubber
outlet stream were 15 ppb, 32 ppb, and 0.6 ppm for AsH3,
PH3, and hydrogen fluoride (HF), respectively.
The monitor's output signal was logged into a computer to enable continuous
monitoring of each scrubber's effluent stream. In some instances, the
FTIR spectrometer was also used to analyze the scrubber exhaust, to
corroborate the measurements collected using the portable monitor. Absolute
pressures before and after the scrubber were measured using pressure
transducers and were logged at 1-second intervals in order to provide
time-dependent pressure characterization. Also, a 01-in.H2O
pressure differential magnehelic gauge provided precise pressure-drop
information across the scrubber.
 |
| Figure 3: External and internal
three-dimensional views of a point-of-exhaust dry scrubber. |
Implanter
Effluent Characterization
Roughing-Pump
Emissions. The effluent gases from all three implanter roughing
pumps were analyzed during ion implantation using AsH3
and PH3 from ATMI SDS sources and high-pressure
BF3 dopant gas. The materials evacuated from the
tool were diluted with nominal 10.2-, 11-, and 6-std L/min nitrogen
flows contributed by the ballasts of the RP1, RP4, and RP2 dry pumps,
respectively (see Figure 1). Three standard recipes covering a wide
range of tool operation parameters were tested for each gas source used.
Prior to running implant processes, the analyzer was calibrated in situ
by measuring the concentration of the gases emitted from the source
chamber pump (RP1) at different flow rates with the beam off.
 |
| Figure 4: Source chamber emissions
through roughing pump RP1 during calibration and implantation of
AsH3. |
During
arsine implantation, small yet measurable levels of AsH3
were detected at the exhaust of the source-chamber roughing pump, as
seen in Figure 4. (Respective parameters for beam energy, beam current,
and gas flow for the three recipes used in this testing were 200 keV,
300 µA, and 1.8 std cm3/min; 2 MeV, 600 µA, and
1.5 std cm3/min; and 90 keV, 11 mA, and 2.2 std cm3/min.)
As observed in previous studies, the unstable beam conditions occurring
during the beam-tuning stages resulted in concentration spikes.1,2
Once the ion beam stabilized, AsH3 concentrations
of up to 1.8 ppm (more than 35 times arsine's TLV) were detected. Levels
of emitted AsH3 increased with beam energy and
flow rate.
 |
| Figure 5: Source chamber emissions
through roughing pump RP1 during calibration and implantation of
PH3. |
After
implantation using arsine, the tool was purged with an argon beam and
tests using phosphine began. The recipes used in that testing were 200
keV, 400 µA, and 2.5 std cm3/min; 1 MeV, 550 µA,
and 2.8 std cm3/min; and 90 keV, 1 mA, and 1.9 std cm3/min.
As had occurred with AsH3, some PH3
exited the tool through the source pump during implantation, as shown
in Figure 5. Up to 20 ppm of the gas (corresponding to more than 65
times phosphine's TLV level) were detected initially, but emissions
later stabilized near 10 ppm.
High-pressure
BF3 was the last dopant selected for characterization.
In this case, the three beam energy, beam current, and gas flow process
recipes were 1 MeV, 1 mA, and 2.8 std cm3/min; 200 keV, 500
µA, and 3.0 std cm3/min; and 90 keV, 1 mA, and 2.6 std
cm3/min. In contrast to the hydride gases, a large percentage
of the BF3 gas delivered into the tool was evacuated
through roughing pump RP1, as illustrated in Figure 6. Concentrations
approaching 300 ppm (95% of the total volume of delivered gas) were
detected. A nearly constant level of 1015 ppm of HF was also measured
during BF3 calibration and implantation. The ratio
of BF3 emitted through this pump to the gas-delivery
rate decreased with increasing beam energy.
 |
| Figure 6: Source chamber emissions
through roughing pump RP1 during calibration and implantation of
BF3. |
The
striking difference between hydride and acid emissions through the source
pump is consistent with previously reported studies.1 This
disparity is independent of the type of implanter (low- or high-current),
suggesting that there is a fundamental relationship between the bond
energies of the individual dopant gases and the levels of gas emission.
Tests
using the same source gases and implant processes were also performed
with the analyzer installed after the beam-line chamber pump (RP4).
As shown in Figure 7, the concentrations of source materials measured
at the exhaust of this pump were typically one to two orders of magnitude
lower than those detected after RP1. The implantation of BF3
resulted in concentrations of approximately 16 ppm of source materials
exiting through the beam-line pump. This value is ~20 times lower than
the BF3 volumes released through the source chamber
pump. Implantation using AsH3 showed an initial
release of 600 ppb of the parent material, with subsequent effluent
levels falling below the detection limits of the analyzer (~100 ppb).
PH3 implant recipes also resulted in an initial
surge in effluent level to 650 ppb), which stabilized to ~350 ppb.
 |
| Figure 7: Beam-line chamber emissions
through roughing pump RP4 during implantation of BF3,
AsH3,
and PH3. |
In
addition, characterization attempts at the exhaust of the RP2 roughing
pump that serviced the process chamber during implantation using the
various gas-flow recipes failed to measure any dopants or hazardous
by-products. The emissions data for roughing pumps RP1 and RP4 are summarized
in Table II.
|
Test
No.
|
Implant
Conditions and
Dopant Delivery Information
|
Emissions
Data Measured at
the Exhaust of Pump
|
Source
Utilization
by Tool
(%)b
|
|
Gas
Source
|
Gas
Flow
Rate (std
cm3/min)
|
Beam
Current
(mA)
|
Beam
Energy
(MeV)
|
Source
Gas in
Mass Rate
(mg/min)
|
RP1
(Source)
Pump
|
RP4
(Beam-line)
Pump
|
|
Avg.
Concen.
(ppm)
|
Total
Mass
Emitted
(mg)a
|
Avg.
Concen.
(ppm)
|
Total
Mass
Emitted
(mg)a
|
|
0
|
AsH3
|
1.8
|
Beam
auto tune
|
5.85
|
2.6
|
0.666
|
Not
measured
|
98.58
|
|
1
|
AsH3
|
1.8
|
0.3
|
0.2
|
5.85
|
0.4
|
0.0829
|
0.0215
|
3.3
X 103
|
99.72
|
|
2
|
AsH3
|
1.5
|
0.6
|
2.0
|
4.88
|
0.163
|
0.0441
|
0.12
|
0.0282
|
99.88
|
|
3
|
AsH3
|
2.2
|
11.0
|
0.09
|
7.15
|
1.11
|
0.158
|
0.0166
|
2.62
X 103
|
99.35
|
|
4
|
PH3
|
2.5
|
0.4
|
0.
|
3.54
|
12.2
|
1.07
|
0.35
|
0.035
|
94.84
|
|
5
|
PH3
|
2.8
|
0.55
|
1.0
|
3.97
|
9.5
|
0.697
|
0.38
|
0.0181
|
96.41
|
|
6
|
PH3
|
1.9
|
1.0
|
0.09
|
2.67
|
6.5
|
0.189
|
0.38
|
0.017
|
93.14
|
|
7
|
BF3
|
2.8
|
1.0
|
1.0
|
7.91
|
256.4
|
20.9
|
6.2
|
1.78
|
8.11
|
|
8
|
BF3
|
3.0
|
0.5
|
0.2
|
8,48
|
289.6
|
39.6
|
7.5
|
1.89
|
3.32
|
|
9
|
BF3
|
2.6
|
1.0
|
0.09
|
7.34
|
258.4
|
21.2
|
7.9
|
1.99
|
3.09
|
aMass
totalized (integrated) over each test time period.
bThis value was computed by comparing
the combined RP1 and RP4 emissions with the dopant delivery
rate. |
|
| Table II: Summary of implanter
conditions and emissions data for roughing pumps RP1 and RP4. |
Cryo-Pump
Regeneration Emissions. The volumes and types of materials trapped
inside cryo pumps depend on the time elapsed since the last regeneration,
the tool utilization rate, and the flow rate and nature of the dopants
being implanted. In this study, the P2 and P9 cryo pumps for the 200-mm
implanter were regenerated 30 days before the test data, and the P3
pump was vented 13 days before the testing. Based on the tool operator's
estimation that the implanter was typically active for 6 hours a day
5 days a week, the elapsed time was 132 hours for the P2 and P9 pumps
and 60 hours for pump P3. These cryo-pump loading periods would correspond
to just 5.5 days and 2.5 days in a typical manufacturing tool operating
in a 24/7 environment. The volumes and types of dopant gases used since
the last regenerations were unknown.
To
measure emission levels separately during testing, cryo-pump regenerations
were triggered manually one pump at a time. The bulk of the gas streams
was composed of dry nitrogen, which is commonly used to vent cryo pumps.
N2 flow rates of 200, 205, and 185 std L/min were estimated
from the pressure drop across the scrubbers for the P2, P3, and P9 pumps,
respectively. Gas-phase analyses during cryo regeneration detected parts-per-million
levels of PH3 and sulfur hexafluoride in addition to water,
CO, and CO2. The concentration-versus-time curves were integrated
to determine the total volume and mass released by each pump. These
values are summarized in Table III.
The
relatively low levels of hazardous materials detected in this part of
the study were not surprising considering the relatively small loading
of the cryo pumps and the high N2 dilution factors.
A more representative study of cryo-pump emissions should be performed
on an ion implanter that had been loaded to manufacturing-like levels.
Effluent
Abatement Tool Efficiency
Conventional
dry scrubbers used for abating ion implantation processes can be categorized
as end-of-pipe or point-of-use (POU), depending on their size, location,
and flow capacity. Typical POU scrubbers are placed adjacent to the
implanter and treat the combined effluents of all roughing and cryo
pumps. Pressure-drop considerations typically limit the flow through
these scrubbers to <15 cu ft/min. On the other hand, end-of-pipe
scrubbers are larger, typically installed remotely, and designed to
process >100 cu ft/min of flow with a low pressure drop.
The
new generation of dry scrubbers investigated in this study were designed
to be installed at the exhaust of each separate pump of an implanter.
Compared to end-of-pipe and POU systems, these point-of-exhaust scrubbers
do not require expensive floor space or routing of exhaust lines. The
results of their performance testing are presented below. Relative pressure
data are reported in the familiar unit, inches of water (in.H2O).
Pressure-Drop
Performance. Excessive flow constriction through a dry scrubber
can result in potentially damaging pressure buildup. Pressurized exhaust
lines can trigger pressure switches that shut down pumps or induce leaks
of hazardous substances through faulty connections or fittings. Pressure
drop is related to the flow rate through the system, among other factors.
In an implanter tool, the exhaust of a roughing pump has a typical flow
rate of 1070 std L/min of inert gas ballast. More detrimental
to pressure drop, however, are the large volumes of gases that are vented
when the tool chambers are evacuated. During these short-lived pumpdowns
from atmospheric pressure, pump throughputs can peak at the nominal
pump capacity. For example, a 2800-std L/min flow can occur when using
a 100-cu ft/min pump. As opposed to roughing pumps, cryo pumps only
vent their contents during regeneration, but during those events, nitrogen-purge-gas
flow rates can exceed 200 std L/min.
|
Emission
Type
|
P2
Pump
|
P3
Pump
|
P9
Pump
|
|
Volume
(cm3)
|
Mass
(mg)
|
Volume
(cm3)
|
Mass
(mg)
|
Volume
(cm3)
|
Mass
(mg)
|
|
CO
|
4.19
|
4.89
|
0.92
|
1.07
|
0.17
|
0.20
|
|
CO2
|
33.3
|
61
|
73.6
|
135
|
29.3
|
53.7
|
|
PH3
|
5.8
|
8.2
|
10.9
|
15.5
|
3.72
|
5.27
|
|
SF6
|
0.79
|
4.8
|
0.02
|
0.10
|
0.01
|
0.08
|
|
H2O
|
1540
|
1155
|
3364
|
2523
|
1290
|
967.3
|
|
| Table III: Summary of cryo-regeneration
emissions data. |
Pressure
drop across the respective scrubbers was measured under typical process
conditions as well as during pumpdowns of the source, beam-line, and
process chambers that were performed using the three separate 35-cu
ft/min roughing pumps. The pumpdown measurements were repeated twice,
with and without the use of an AutoSoft flow-dampening device from MKS
Instruments (Andover, MA). Such devices, which are installed in-line
before the pump, consist of a flap gate that automatically shuts under
excess flow conditions and opens during normal flow conditions. The
facilities draw provided a negative pressure with respect to the room
environment (measured at the outlet of the scrubber) of 2.14 in.H2O.
The
test results indicated that the pressure drops across the scrubbers
during regular process conditions were low, ranging between 0.005 and
0.02 in.H2O, depending on the pump being used.
As expected, pressure drops increased momentarily during pumpdowns because
of the brief spikes in gas-flow rates. Without the use of the flow-dampening
device during chamber pumpdown, maximum transient pressure drops of
4.2 and 2.7 in.H2O were measured across the scrubbers
installed after the beam-line and source chamber (RP4 and RP1 pumps,
respectively). Use of the dampening devices reduced these pressure-drop
spikes by approximately an order of magnitude. Figure 8 depicts the
time-dependent pressure at the inlet and outlet of the RP4 scrubber
during pumpdown of the beamline chamber.
 |
| Figure 8: Time-dependent characterization
of the pressure drop across the scrubber installed following pump
RP4 during pumpdown of the beam-line chamber, with and without a
flow-dampening device. |
The
pressure drop across the scrubber that simultaneously treats the exhaust
streams of all three cryo pumps was also characterized. Regeneration
of each cryo pump was triggered manually to capture the individual pressure-drop
contributions; the resulting pressure drops across the scrubber were
similar, averaging 0.37 ± 0.002 in.H2O. All
three cryo pumps were also regenerated simultaneously, resulting in
a pressure drop across the scrubber of 0.91 in.H2O.
Abatement
Performance. To evaluate scrubber efficiency, FTIR spectroscopy
(for the scrubber inlet) and portable gas monitors (for the scrubber
outlet) were used during implant processing using standard recipes and
AsH3, PH3, and BF3
sources. Test conditions included the delivery of up to 5 std cm3/min
of dopant gases into the scrubber with the ion beam off. This challenge
was sustained for at least 10 minutes for each gas. Throughout this
part of the study (in tests involving all roughing and cryo pumps),
no chemical breakthroughs were detected. Scrubbing efficiencies of >99.995%
were achieved during the full hydride challenge (a 310-ppm inlet concentration
was reduced to <0.015 ppm at the outlet). Similarly, efficiencies
of >99.8% were derived for BF3 (a 410-ppm inlet
concentration was reduced to <0.6 ppm at the outlet). Confirmation
of the scrubber efficiency data was obtained by measuring the scrubber
exhaust using the FTIR spectrometer while delivering maximum flow rates
of AsH3, PH3, and BF3,
with the beam off.
 |
| Figure 9: Results of periodic pressure-drop
characterization of various scrubbers during normal operation, pumpdown,
and cryo regeneration. |
Long-Term
Scrubber Performance. Since their installation, the performance
of the scrubbers has been monitored periodically to provide comprehensive
data on their capabilities over time. A 10-month summary of the pressure
drop across the systems during normal operation, pumpdown, and cryo
regeneration is provided in Figure 9. In all of these tests, the roughing
pumps were equipped with flow-dampening devices. The periodic measurements
of the scrubber exhaust gases revealed no breakthroughs, indicating
that the units continued to abate all toxic gases from the implanter.
Additional
long-term scrubber performance data have been provided by Atmel (Beverly,
MA), where 30 of the units were installed in mid-2000. Similar to Axcelis's
installation, all of these scrubbers are placed on top of implanters
to abate the effluent gases from roughing and cryo pumps. In this manufacturing
environment, the end-user reported that units installed on high-current
implanters have a typical lifetime of 612 months, while those
installed on medium-current tools have a lifetime in excess of 1 year.
Conclusion
Ion
implantation processes emit materials that are potentially hazardous
to humans and the environment. While the effluent characterization study
presented here revealed that measured absolute concentrations of dopant
gases are small, the levels relative to their respective safety thresholds
were found to be significant. Comparison of this project's results with
those of other emission studies suggests that the frequency and intensity
of vented gases are independent of the type of tool used (high-energy
versus high-current). Instead, gaseous emissions are correlated to the
dopant being implanted (hydrides or acid materials), implanting parameters
(dopant flow rates, beam energy, and beam current), type of pump (roughing
or cryo), and location of the pump within the tool.
The
performance of dry scrubbers dedicated to abating implantation tool
effluent was also studied. Compared with conventional methods of pollution
control, these small devices simplify the abatement process by allowing
easy installation at the exhaust of each implanter pump without requiring
an additional equipment footprint. Periodic monitoring revealed that
the units can provide from 6 to 12 months of service, depending on implanter
type and uptime. In performance tests, the pressure drop across the
devices was typically <1 in.H2O during normal
operation; during pumpdown of the entire tool, short transient pressure
drops reached 4 in.H2O. No chemical breakthroughs
occurred during the study, and scrubber efficiences were measured at
>99% for the three dopants used in the testing.
Acknowledgments
The
authors would like to acknowledge the assistance of Rob Spreng, who
operated the ion implanter during the characterization study and the
ensuing performance scrubber tests at Axcelis. In addition, special
thanks go to Chad Ramirez of Atmel for providing information on the
performance of Novasafe scrubbers installed at that facility.
References
1. J
Arnó et al., "Hazardous Gases Emitted by Ion Implanters; Characterization
and Abatement," Solid State Technology 41, no. 10 (1998): 113120.
2. B
Goolsby et al., "Analysis of Implanter Source-Region Exhaust by FTIR,"
in Proceedings of the Electrochemical Society, vol. 20016
(Pennington, NJ: Electrochemical Society, 2001), 5967.
Josep
Arnó, PhD, is a director of R&D at Advanced Technology
and Materials (ATMI) in Danbury, CT, where he is responsible for the
development of innovative abatement methods and the safe packaging of
semiconductor materials. He has research experience in molecular spectroscopy,
computational quantum mechanics, and plasma abatement. Arnó has
authored more than 20 publications in the areas of front-end and back-end
semiconductor materials handling and processing. He received a PhD in
physical chemistry from Texas A&M University in College Station.
(Arnó can be reached at 203/207-9304 or jarno@atmi.com.)
Joseph
Sweeney is R&D manager for the treatment group of ATMI. He has
seven years of experience in the semiconductor industry and has focused
primarily on the development of new abatement products. He received
bachelor's degrees in chemical engineering and chemistry from the University
of Wisconsin in Madison and is working toward a masters degree in mechanical
engineering from the Georgia Institute of Technology in Atlanta. (Sweeney
can be reached at 203/207-9364 or
jsweeney@atmi.com.)
Paul
Marganski is a research engineer at ATMI. For the past three years,
he has been developing novel methods for improving hazardous materials
abatement in ion implant, III-V MOCVD, and metal etch. In addition,
he has been working on wet bench exhaust reduction. Prior to joining
ATMI in 2000, Marganski worked for the chemical process design group
at Cytec Industries in Wallingford, CT. He received a BS in chemical
engineering from the University of New Haven in Connecticut. (Marganski
can be reached at 203/739-1464 or pmarganski@atmi.com.)
Brian
Kingston is marketing manager for the treatment group at ATMI, a
position he has held for four years. Previously, he was in customer
support at IBM in New Zealand and at Honeywell in the UK. He received
a BS in business and is pursuing an MBA in marketing at Phoenix University.
(Kingston can be reached at 408/933-3518 or bkingston@atmi.com.)
Steven
Roberge is the global environmental health and safety (EHS) and
product stewardship manager at Axcelis Technologies (Beverly, MA). He
is involved in all aspects of EHS management and product stewardship
for ion implanters, rapid thermal processors, and cleaning and curing
systems. Roberge has authored several papers and presentations on various
aspects of semiconductor EHS and has contributed to the safety chapter
of the Ion Implant Science and Technology Handbook. He received a BS
in environmental science from the University of Massachusetts in Amherst.
(Roberge can be reached at 978/787-9889 or steve.roberge@axcelis.com.)
M.
Christopher Dolan is high-energy engineering product manager at
Axcelis, where he has worked for eight years. He received a BS in mechanical
engineering from Northeastern University in Boston. (Dolan can be reached
at 978/787-4000 or chris.dolan@axcelis.com.)