Title: CIC Photonics
1CIC Photonics
2Schedule - Day 1
- FTIR analysis
- IR spectrum
- Michelson interferometer
- Fast Fourier transform and corrections
- Interferogram, single beam spectrum, absorption
spectrum and transmission spectrum - Beers law
- Instrument resolution
- Quantification analysis-Classical Least Squares
introduction - Hardware description
- Bomem WorkIR
- Instrument purge
- Manual manifold
- SPGAS software
- IRGAS 100
- IRGAS configuration manager
- Data retrieval
3Schedule - Day 2
- SPGAS software cont.
- Qmax quantification manager
- IRGAS spectra reprocessing software
- Hardware installation
- System power
- Pipe installation
- Instrument purge
- Software installation
- IRGAS software
- Bomem Ethernet drivers
- System verification
- System maintenance
4Schedule - Day 3
- IRGAS worksheet
- IRGAS options
- IRGAS product array
- Marketing and selling strategies and techniques
- Competitors and competing products
- Service and maintenance
5FTIR Analysis
6Light Spectrum
- Infrared is invisible light ranging from 1mm to
750nm in wavelength - Infrared light can be divided into three parts
- Far infrared -1mm to 10µm
- Mid infrared - 10µm to 2.5µm
- Near infrared - 2.5µm to 750 nm
7Infrared (IR) Spectrum
- IRGAS System mid infrared range
- 2.5µm 25µm in wavelength
- 4000 cm-1 400 cm-1 in wavenumbers
- Wavelength (?)
- Wavelength (1/wavenumber)10,000
- Wavenumber (cm-1)
- Wavenumber (1/?)10,000
8IR Molecules
- Not every molecule absorbs infrared light
- Monoatomic
- He, Ar, Ne, etc
- Homoatomic diatomic
- N2, O2, H2, etc
- N N
- Molecules that do absorb infrared light
- Water is a good example
-
- O
- H H
9Michelson Interferometer
2
1
3
4
- Step 1 Beam leaves IR source and hits
beamsplitter where it is sent straight through
and at a 90 angle - Step 2 The 90 angle beam hits a fixed mirror
and is sent back to the beamsplitter - Step 3 The beam that went straight through hits
a movable mirror and is sent back to beamsplitter - Step 4 The two beams recombine, go through the
gas cell and travel to the detector
10Michelson Interferometer
- When ABAC the phase of the frequencies look the
same - When ABAC1/4?, then the phase of the
frequencies are opposite in regards to maximums
and minimums
11Michelson Interferometer
- When ABAC and the two recombine you get stronger
maximums and minimums - When ABAC1/4? and the two recombine they cancel
one another out and result in a flat line
12ABB Bomem Michelson Interferometer
- It has two sets of mirrors that move by a
pivoting motion - This design is called a wishbone configuration
- This configuration is more robust
- It can be placed in any orientation
- This configuration only has to be smooth at one
point vs. the traditional interferogram that has
to be smooth along a rail
13ABB Bomem Michelson Interferometer
14ABB Bomem Michelson Interferometer
Laser
15Fast Fourier Transform
- The highest peak intensity is attained when ABAC
- The maximum of the highest intensity peak is
called the zero path difference (ZPD) point - After the interferogram has been created by the
instrument, the Fourier transform is applied to
it, which then results in a single beam spectrum
16Single Beam Spectrum
17Single Beam Spectrum
18Single Beam Spectrum
19Single Beam Spectrum
20Transmission
- The ratio between the sample and the background
spectrum
21Transmittance Spectrum
22Chemometrics
- Based on the transmission spectrum chemometrics
can be applied - Chemometrics The application of statistical and
mathematical methods for the design or
optimization of chemical experiments and for the
efficient extraction of information from chemical
data - Two types of chemometrics
- Qualitative (identification)
- Quantitative (quantity)
23Absorbance
24Beers Law
- Says that concentration is directly proportional
to absorbance (linearity) - Beers law equation is A abC
- Where A absorbance
- a absorptivity of the molecule
- b pathlength that the light travels
- C concentration
25Instrument Resolution
- The more points per peak the higher the
resolution - The higher the resolution the more noise, but the
better peak separation - Common resolution used for an ABB Bomem
instrument is 2 cm-1 - Ranges between 1 cm-1 to 128 cm-1
26Why Do We Need a Gas Cell
- Intensity of a peak is directly related to the
of moles in a sample - In the same area
- Solid will be very packed
- Liquid will be less packed
- Gas will be even less packed
27Long Path Gas Cell
284Runner 6 Meter Gas Cell
29Gas Cell Mirrors
Top view of field mirror
30IR Beam Path
31Classical Least Squares (CLS)
- The base equation is As AcK e
- Where As sample absorption
- Ac calibrated absorption
- K concentration
- e noise
- Using the above equation find K that minimizes e
- To minimize e we use the CLS method
- In this situation there are more equations then
variables
32Classical Least Squares (CLS)
- To simplify matters we assume that e 0
- The equation then becomes As AcK
- Matrix form
33Classical Least Squares (CLS)
- In order to solve for K (Ac-1As K), Ac needs
to be an inverse matrix - Therefore AcTAs (AcTAc)K
- (1x1) (1x1)K
34Problems with Initial CLS Approach
- Baseline becomes unstable throughout the day
- It can shift, slope, or curve
- These changes can be compensated for in the
calibrated absorption matrix
35Classical Least Squares (CLS)
- Accounting for these baselines changes the
equation - The eqn. becomes As AcK1 K2 K3
K4 - The calibrated absorption matrix can be increased
to accommodate the number of species being tested
36Weighted Multi-band CLS
- A more complex version of the standard CLS
- The spectrum is separated into bands
- Each band is then calculated
- After all the bands are calculated they are added
in a weighted averaged fashion - The ones with the highest error and lowest signal
are counted for less then the ones with the
lowest error and highest signal
37Hardware Description
38IRGAS Systems
- Thus far the oldest system in the field without
maintenance is 4 yrs - Out of 20-30 systems, there has only be a need to
perform maintenance on 3 of them - The Bomem spectrometer is high in reliability and
low in maintenance - There has been 2 hardware failures
- There was a burned out IR source
39IRGAS Systems
- There is one basic package that can be dressed up
in several different ways - One reason our throughput is higher than
competitors is because of mirror quality and
coating - Our objective mirrors are adjustable
- Sideways
- Rotational
- Competitors have mirror that are locked into
place
40ABB Bomem WorkIR
41Manual Manifold
42Manifold Parameters
- Flow Restrictor
- A flow of 30 psi in will give a flow of 5 slpm to
the instrument - Purifier
- Gives dry N2 to below 2 ppb
- Has a lifetime of more than a year if it is used
24/7
43Vibrations
- There are a number of designs of suspension
systems to counteract vibrations - These designs help to keep the data from being
affected by a simple bump of the instrument bench
44Typical Gas Cells
- Have a flow similar to turbulent flow and have a
longer residence time
45Laminar Flow Gas Cells
- The flow is like a waterfall
- Therefore there will be less turbulence
- Heated laminar flow gas cells
- The gas is in contact with the walls letting it
reach a temperature similar to the gas cell prior
to entering the cell
46Gas Cell Flow Diagrams
47f/5 Beam Geometry
- The higher the f / , the smaller the objective
mirrors, the more light that is lost, the smaller
the throughput
48SPGAS Software
49Specialty Gas Analysis Software (SPGAS)
- IRGAS 100 system
- Collection quantification
- Qmax
- Quantification manager
- IRGAS Configuration Manager
- Configures parameters
- Quantification Reprocessing Tool
- Recalculating spectra
50IRGAS 100 System
- After opening the software the first window is
the monitor screen - On the right side there is the available species
- On the bottom is the legend of the species that
are being shown in the top window - The top shows the concentration of all the
species over time
51IRGAS 100 Monitor Screen
52IRGAS 100 System
- Collecting a background
- After opening the program, pressing the start
button will automatically send the spectrometer
to collect a background and then begin collecting
a sample - Seeing the sample
- Clicking on the desired species tab at the top
will show you that species in real time - That screen shows the fast concentration tracker
(FCT) and the averaged sample
53Advantages to Spectra Stream
- Provides high sensitivity detection of impurities
(low ppb) - Reduces the time response typically associated
with FTIR (from minutes to seconds) - Continuous collection of background
- Running average spectra
- Reduction in spectrometer drift
- Reduction of contribution of moisture
- System is very easy to use
54IRGAS Configuration Manager
55IRGAS Configuration Manager
56IRGAS Configuration Manager
57IRGAS Configuration Manager
58IRGAS Configuration Manager
59 Data Retrieval
- Data storage
- By default the data gets stored on the C drive
- C\Program Files\CIC Photonics\IRGAS
- IRGAS data
- Quantification log
- Spectral records
60Quantification Log Folder
- Data stored as a text file
- Can be converted to an excel file
- Copy file, paste in the same folder, rename with
an .xls extension - In the excel file
- Data storage names
- Folder with YY-MM
- Folder with Quan YY-MM-DD.log
61Spectral Records Folder
- Stored with a .spc extension
- All market software writes and reads this format
- This was created by Galatic, now ThermoGalactic
- Data storage names
- Folder with YY-MM-DD
- Absorbance File
- Abs YY-MM-DD HHMM.zip
- Background File
- Bck YY-MM-DD HHMM.zip
- Sample File
- Smp YY-MM-DD HHMM.zip
- Residual File
- Res YY-MM-DD HHMM.zip
62QMax
- Using existing calibration file
63QMax
Quantification Set
Spectral Set
Calibrated Spectral Record of specific molecule
64Non-linear Behavior
- As a rule of thumb a species behaves non-linear
when it is higher than 0.1 a.u. - The non-linear correction graphs curve is
modeled by ax3bx2cxd 0 - In this equation the values that are necessary to
find are a, b, and c - To do this non-linear correction there needs to
be at least 3 spectral records - In general when the residual curve is flat line
that indicates that there is non-linear behavior
65QMax
- Starting a calibration from scratch
66Synthetic Calibration Set
- Instrument Line Shape (ILS)
- Each instrument has its own
- HITRAN database
- Contains the absorption coefficients of different
components - Doesnt contain the ILS of specific instruments
- MALT software
- Created by Dr. David Griffith from the University
of Wollongong in Australia - Models ILS parameters
67MALT
- Calculates spectra for single homogeneous path or
for multiple layers - Includes instrumental parameters into the
calculations so the calculated spectra match the
line shape, resolution and wavelength shift of
the measured spectra - Uses HITRAN molecular spectroscopy databases
68Gas Calibration
- When a gas is not in the HITRAN system, it is
necessary to produce the calibration
non-synthetically - Start collecting data
- Flush the gas cell several times with the gas
- During this time find the equilibrium point of
each flush - Take these points and average them to use for the
calibration - This will give a better signal to noise ratio
69HITRAN/MALT vs. Actual Calibration
- Advantages
- Calibration data free of noise
- Best match to the measured spectrum according to
the least squares criteria - Operational costs reduction
- Non-time consuming calibrations
- Precision at least as good as that of traditional
methods ( ? 3)
70HITRAN/MALT vs. Actual Calibration
- Disadvantages
- Provides analysis only over gases included in the
HITRAN database - System requires regeneration of calibration data
if spectrometer or gas cell change
additional gases by standard calibration
procedures
71IRGAS Spectra Reprocessing
72IRGAS Spectra Reprocessing
73Gas Analysis Modules
74Absorbance Data _at_ 1ppm/meter
75Software Installation
76Software Installation
- The installation window should automatically
pop-up - After the installation has been completed, check
that the computer and spectrometer are
communicating with each other
77Establishing Communication
- Network
- Instrument address 192.168.0.127
- Computer address 192.168.0.YYY
- Where YYY is any number between 0 and 225 that is
not 127
78Establishing Communication
- Two Ethernet configurations
- Straight through
- Crossover
79Ethernet Connection
- Straight through configuration
- 1 1
- 2 2
- 3 3
- 4 4
- 5 5
- 6 6
- 7 7
- 8 8
80Ethernet Connection
- Crossover configuration
- 1 1
- 2 2
- 3 3
- 4 4
- 5 5
- 6 6
- 7 7
- 8 8
81Verifying Communication
- Changing network address
- Control panel
- Network connection
- Local network
- Properties
- Last check for communication
- Control panel
- ABB Bomem
82Marketing and Selling Strategies and Techniques
83Worldwide Customers
84Semiconductor Applications
- Wafer yield enhancement
- By reducing O-atom defects
- Process reaction monitoring
- By confirming reactants/products
- Supply gas quality monitoring
- Abatement tool efficiency
85Semiconductor Dry Process
http//www.jp.horiba.com/semicon_e/measurement/gas
.htm
86Semiconductor Industry
87Semiconductor Applications
- A large amount is spent on equipment in the fab
area - In-situ monitoring is being looked at to prevent
the damage of large quantities of goods - The equipment section is also supplying the raw
materials section, not just the Semi fab - Getting the companies to upgrade current
equipment is difficult but results is a large
sale
88Chemical Applications
- Specialty gas purification
- Combustion thermodynamics
- Aero-engine optimization
- Destructive testing release of hazardous gases
- Gas blending
89Environmental Applications
- Plant air monitoring
- Stack gas emissions
- PFC emissions
- Homeland Security
- Chemical Weapon Agents
- Toxic Industrial Chemicals
- Illicit Drugs
90Our Product Line
- FTIR gas analyzer systems
- Long and short path gas cells
- Custom gas cells
- Fiber optic probes (UV/VIS/NIR)
- Resell UV/VIS FO spectrometers
- FTIR sampling accessories
- ATR, transmission, reflectance, M-Press
91Competitor Analysis
Research conducted by Los Alamos National
Laboratories marketing interns
92Competitors and Competing Products
93Competitors
- FTIR gas analyzers
- MKS Instrument
- MIDAC
- Thermo Nicolet
- Other technologies
- Tiger Optics
- Delta F
94Other Technology Competitors
- Tiger Optics
- Cavity Ring Down Spectroscopy (CRDS)
- Single gas at a time
- Delta F
- Tunable laser
- Single gas at a time
95Differentiators
96Gas Cells
- Laminar flow
- Faster gas exchange
- Eliminates dead space
- 316L Stainless steel / Nickel plated body
- More chemically resistant to acid gases and
retain less moisture - 304 Stainless steel mirror
- Proprietary fabrication and coating process
- Radius of curvature
- Surface finish smoothness
- 98.5 reflectivity
- High pressure tolerance
- 20 atm, 300 psi
- Hand aligned by expert personal to maximize
throughput
97IRGAS System
- Spectrometer
- ABB Bomem WorkIR
- Industrial ruggedness
- Compactness
- Very low failure rate
- Cost competitive
- Software
- Unique because it offers the weighted multi-band,
multi-variant classical least squares method - Patented on Spectra Stream w/ the fast tracker
for early warning - User friendly
- Configurations
- One package that can be dressed different ways
- Pre and post technical support
98Scientific Package
- 4Runner gas cell
- ABB Bomem WorkIR spectrometer
- Coupling optics
- Suspension system
99The 4Runner
- 0.6 liter volume
- 125 mm base path
- 304 stainless steel body
- Metal and Kalrez seals
- Welded VCR fittings for gas porting
- Heatable to 260C
- Integrated purge box with movable reference
optics - MgF2 protected, gold-coated stainless steel
mirrors - Evacuable pressurizable 10-4 Torr to 300 psig
100Ranger-EN
- 9.6 meter fixed pathlength
- 1.7 liter cell volume
- 0.05 sq. m/L surface/volume
- Gold-coated SS mirrors
- All-metal, electropolished SS body
- External transfer optics
- Heatable to 200C
- Optional aluminum body glass mirror
101Pathfinder-EN
- 0.4-10 meter variable pathlength
- Pressurizable to 50 psig
- Heatable to 200C
- Gold-coated SS mirrors
- All-metal, electropolished SS body
- Very high energy throughput
- Extremely chemically-inert
102Scout-EN
- Nickel plated stainless steel 10cm gas cell for
toxic and corrosive gas analyses heated and
unheated versions. - 28-cm3 volume
- Teflon-encapsulated Viton, Viton, or Kalrez
O-rings for chemical resistance and temperature
considerations - KBr, CaF2, ZnSe, quartz, or sapphire window
materials for UV-VIS and FTIR applications - Evacuable and pressurizable 10-4 Torr to 150
psig - Heatable to 200C with heating mantle, tape, or
dual bands - 5 cm 15 cm pathlength versions also available
- Optional temperature controller
- Easy adaptation to all spectrometers
103Montero
- 1.0 meter fixed pathlength
- 82.6 mm basepath
- Anodized aluminum cell body
- Gold-coated Pyrex mirrors
- Internal transfer optics
- Low 600 ml volume
- Purgeable beam conduits
- Swagelok (tm) gas ports
- Viton O-rings
- Choice of windows
- High energy throughput
- Unheated and heated versions
- Fits totally inside FTIR compartments
104CR-V
- Extremely short path length
- 0.5mm to 1cm
- High Pressure
- Up to 100 atm
- Heated Option
105IRGAS Options
106O-Ring Material Working Temperature Ranges
107Window Thickness
108Options
- Pressure and temperature based on ideal gas
parameters - Automated manifold systems
- System outputs
- Text based
- Analog and digital outputs
109IRGAS Moisture Plus
110IRGAS-SP
111IRGAS EPI
112IRGAS 100T
113IRGAS 100MT
114IRGAS 200RM
115IRGAS 400
116IRGAS XFlo
117IRGAS Worksheet
118IRGAS Worksheet
- Important because it guides us in system
parameters, options, and price quoting - Important parameters
- Gases present in the mixture
- Estimated concentrations
- Temperature and pressure range
- Sampling time
- The parameters help to determine
- O-Ring material
- Window material
- Gas cell
- All of these can really vary the price of the
product
119IRGAS Worksheet
- Part A of the worksheet is for customers that
only want a gas cell - The entire worksheet is necessary for customers
that want the whole IRGAS system - Customers should fill out as much of the
worksheet as possible
120Warranties and Technical Support
121Warranty
- 1 yr parts and labor for gas cell and software
- 30 day on critical optical elements, ex. mirrors
- This is because we have no control over how the
system is treated by the user - 1 yr telephone and e-mail technical supprt
122Technical Support
- 24/7 technical support is provided to the best of
our abilities
123System Maintenance
124Service and Maintenance
- Handled on a case to case basis
- Repair, test, ship
- System repaired
- Quality tested
- Shipped back to customer
- CIC Photonics pays the shipment back to customer
if still under warranty, if not it is paid both
ways by the user
125Contact Information (505) 343-1489(505)
343-9520 TechSupport_at_cicp.com