Title: Photolithography, Next Generation Lithography and Future Lithography 5b
1Photolithography, Next Generation Lithography and
Future Lithography (5b)
2Next Generation and Future Lithography
- We categorize emerging lithography tools in next
generation lithographies (NGLs), i.e.,
lithographies beyond deep UV lithography (DUV)
and future lithography approaches in the RD
stage.
3 Next Generation Lithography (NGL)
4Next Generation Lithography (NGL)
5Next Generation Lithography EUV
- Uses very short 13.4 nm light
- All reflective optics (at this wavelength all
materials absorb!) - Uses reduction optics (4 X)
- Step and scan printing
- Optical tricks seen before all apply off axis
illumination (OAI), phase shift masks and OPC - Vacuum operation
- Laser plasma source
- Very expensive system
6Next Generation Lithography EUV
- Mask fabrication is the most difficult task
7Next Generation Lithography E-Beam
- The advantages of electron lithography are
- (1) Generation of micron and submicron resist
geometries - (2) Highly automated and precisely controlled
operation - (3) Greater depth of focus
- (4) Direct patterning without a mask
- The biggest disadvantage of electron lithography
is its low throughput (approximately 5 wafers /
hour at less than 0.1 µ resolution). Therefore,
electron lithography is primarily used in the
production of photomasks and in situations that
require small number of custom circuits.
8Next Generation Lithography E-Beam
- Diffraction is not a limitation on resolution (l
lt 1 Å for 10-50 keV electrons) - Resolution depends on electron scattering and
beam optics the size of the beam, can reach 5
nm - Two modes of operation
- Direct writing with narrow beam
- Electron projection lithography using a mask EPL
- Issues
- Throughput of direct writing is very low
research tool or low pattern density
manufacturing - Projection stepper (EPL) is in development stage
only (primarily by Nikon). - Mask making is the biggest challenge for the
projection method - Back-scattering and second electron result in
proximity effect reduce resolution with dense
patterns there is also the proximity effect - Operates in high vacuum (10-6 10-10 torr) slow
and expensive
9Next Generation Lithography E-Beam
- Electron scattering in resist and substrate
- The scattered electrons also expose the resist
- Interaction of e-and substrate resist leads to
beam spreading - Elastic and in-elastic scattering in the resist
- Back-scattering from substrate and generation of
secondary e- - 100 Å e-beam become 0.2 µm line
10Next Generation Lithography E-Beam
11Next Generation Lithography E-Beam
- Pattern directly written into resist by scanning
e-beam - Device is just like an SEM with
- On-off capability
- Pixelation
- Accurate positioning
- E-beam blur
12Next Generation Lithography E-Beam
13Next Generation LithographyE-Beam
- Thermionic emitters
- Electrons boiled off the surface by giving them
thermal energy to overcome the barrier (work
function) - Current given by Richardson-Dushman equation
- Field Emitters
- Takes advantage of the quantum mechanical
properties of electrons. Electrons tunnel out
when the surface barrier becomes very narrow - Current given by Fowler-Nordheim equation
- Photo Emitters
- Energy given to electrons by incident photons
- Only photo-electrons generated close to the
surface are able to escape
14Next Generation LithographyE-Beam
15Next Generation LithographyE-Beam SCALPEL
(SCattering with Angular Limitation Projection
Electron-beam Lithography)
- EPL is e-beam with a mask for high-throughput
- The aspect of SCALPEL which differentiates it
from previous attempts at projection
electron-beam lithography is the mask. This
consists of a low atomic number membrane covered
with a layer of a high atomic number material
the pattern is delineated in the latter. While
the mask is almost completely electron-transparent
at the energies used (100 keV), contrast is
generated by utilizing the difference in electron
scattering characteristics between the membrane
and patterned materials. The membrane scatters
electrons weakly and to small angles, while the
pattern layer scatters them strongly and to high
angles. - An aperture in the back-focal (pupil) plane of
the projection optics blocks the strongly
scattered electrons, forming a high contrast
aerial image at the wafer plane
16Next Generation LithographyE-Beam SCALPEL
(SCattering with Angular Limitation Projection
Electron-beam Lithography)
- The functions of contrast generation and energy
absorption are thus separated between the mask
and the aperture. This means that very little of
the incident energy is actually absorbed by the
mask, minimizing thermal instabilities in the
mask. It should be noted that, although the
membrane scatters electrons weakly compared to
the scatterer, a significant fraction of the
electrons passing through the membrane are
scattered sufficiently to be stopped by the
SCALPEL aperture. - Mask easier/simpler than EUV
17 Next Generation LithographyE-Beam SCALPEL
(SCattering with Angular Limitation Projection
Electron-beam Lithography)
18Next Generation Lithography x-Rays
- X-ray lithography employs a shadow printing
method similar to optical proximity printing. The
x-ray wavelength (4 to 50 Å) is much shorter than
that of UV light (2000 to 4000 Å). Hence,
diffraction effects are reduced and higher
resolution can be attained. For instance, for an
x-ray wavelength of 5 Å and a gap of 40 µ, R is
equal to 0.2 µ. - Became very important in MEMS LIGA
- Despite huge efforts seems abandoned for NGL for
now
Grenoble Synchrotron
19Next Generation Lithography x-Rays
- Types of x-ray sources
- Electron Impact X-ray source
- Plasma heated X-ray source
- Laser heated
- E-beam heated
- Synchrotron X-ray source
20Next Generation Lithography x-Rays
- Mask Needs a combination of materials that are
opaque (heavy element, e.g. Au) and transparent
(low atomic mass membrane, e.g. BN or S3N4) to
x-rays - Mask written by e-beam
- Diffraction is not an issue (shadowing is, see
next viewgraph) - Masks difficult to make due to need to manage
stress - Dust less of a problem because they are
transparent to x-rays
21Next Generation Lithography x-Rays
- On account of the finite size of the x-ray source
and the finite mask-to-wafer gap, a penumbral
effect results which degrades the resolution at
the edge of a feature. - An additional geometric effect is the lateral
magnification error due to the finite
mask-to-wafer gap and the non-vertical incidence
of the x-ray beam. The projected images of the
mask are shifted laterally by an amount d, called
runout. This runout error must be compensated for
during the mask making process.
22Next Generation LithographyIPL
- Ions scatter much less than electrons so a higher
resolution is feasible - Problems
- Ion Beam source (e.g. Gallium)
- Mask
- Beam forming
- Not as mature as EPL
23Next Generation LithographyIPL
- Ion lithography can achieve higher resolution
than optical, x-ray, or electron beam
lithographic techniques because ions undergo no
diffraction and scatter much less than electrons.
In addition, resists are more sensitive to ions
than to electrons. The Figure below depicts the
computer trajectory of 50 H ions implanted at 60
keV. As illustrated, the spread of the ion beam
at a depth of 0.4 µ is only 0.1 µ. There is
also the possibility of a resistless wafer
process. However, the most important application
of ion lithography is the repair of masks for
optical or x-ray lithography, a task for which
commercial systems are available.
24Next Generation LithographyIPL
25 Future LithographyOverview
- Proximal Probe Writing Techniques with massive
parallel writing arrays Using MEMS tools - Block copolymers
- Zone plate array lithography (ZPAL),
- Quantum lithography (two-photon lithography)
- Lithography with superlenses (Pendrys dream).
26Future LithographyOverview
- SAM and LB films
- Nanoimprint lithography (NIL) and Step-and-Flash
Imprint Lithography (SFIL) - It is quite possible that some of the alternative
lithography tools we treat in the RD category,
will emerge as serious next generation
lithographies (NGL) in the coming years.
27Future LithographyProximal Probes
- Proximal probe techniques rely on the use of
nanoscale probes, positioned and scanned in the
immediate vicinity of the material surface. - Proximal probes might involve
- Electrical methods where a scanning tunneling
microscope (STM) tip generates a local field
/current that modifies the region directly under
the tip (e.g., SiH ? Si). - A second approach involves mechanical methods
where a scanning force microscope (SFM / AFM) tip
scrapes, thermally deforms or transfers material
at the surface, the latter material transfer
method corresponds to dip-pen lithography (DPL). - Thirdly it may involve a near-field optical
scanning microscope (NSOM) tip or apertureless
near-field scanning optical microscopy (ANSOM),
that exposes photoresist under the tip only.
28Future LithographyProximal Probes
- The use of single proximal probe tips poses a
serious drawback in terms of processing speed. To
use these techniques in the actual manufacture of
ICs and data storage devices, it is necessary to
devise a scheme for parallel processing by making
arrays of these proximal probes.
29Future LithographyParallel Writing
- Zlatkin et al., developed an elegant array of
focused electron writing beams operating at 300
eV or less. The emitters used are cold
field-emission (CFE) sharpened tungsten tips,
although thermionic or Schottky emitters would be
feasible as well. The emitters are positioned
several millimeters above the micromachined
extraction holes of a lens array fashioned in a
single crystal substrate. - At Cornells National Nanofabrication Facility
(NNF) A field emission tip is mounted onto an
STM the STM feedback principle is used for
precision x, y, and z piezoelectric alignment of
the tip to a miniaturized electron lens to form a
focused probe of electrons
30Future Lithography Proximal Probe Writing
Techniques
- Proximal probe based techniques such as atomic
force microscopy (AFM), scanning tunneling
microscopy (STM), dip-pen lithography (DPL) and
near-field scanning optical microscopy (NSOM),
and apertureless near-field scanning optical
microscopy (ANSOM). - In dip-pen lithography (DPL) a reservoir of ink
is stored on the cantilever holding the scanning
probe tip, which is manipulated across the
surface, leaving lines and patterns behind.
Lines as thin as 15 nanometers have been drawn.
The attainable resolution depends strongly on the
substrate roughness, the writing speed and the
relative humidity.
31Future Lithography Proximal Probe Writing
Techniques
- A thermal-DPN (tDPN) method was developed by
Georgia Techs William King and NRLs Lloyd
Whitman - By using easily-melted solid inks and special AFM
probes with built-in heaters writing can be
turned on and off at will.
32Future Lithography NSOM and ANSOM Proximal Probes
- To obtain a resolution better than Abbes optical
microscopy limit - complicated and costly electron (0.1 nm
resolution) or scanning tunneling microscopes
(STMs with atomic resolution) are required. - Unfortunately, these techniques do sacrifice many
of the advantages associated with traditional
optical microscopes (non-destructiveness, low
cost, high speed, reliability, versatility,
accessibility, ease of use, informative contrast,
spectroscopy and real time). - Combining a scanning proximal probe technique
with optical microscopy in so-called scanning
near-field optical microscopy, NSOM provides an
attractive solution to this dilemma.
33Future Lithography NSOM and ANSOM Proximal Probes
- In NSOM, the sample is illuminated by a
nanoscopic light source located close to the
surface (10 nm) and the resolution is dictated by
the source diameter a or - This is achieved by using nanoscale apertures in
NSOM or by using aperture-less techniques in
apertureless near-field scanning optical
microscopy (ANSOM) or scattering SNOM.
34Future LithographyPlasmon Lithography
- Plasmonics Using local field enhancement
occurring around metal nanoparticles when they
are excited at the surface plasmon resonance
frequency can be used to print nanoscale features
in thin resist layers. - Feature sizes below ?/10 were generated in a
parallel fashion using visible illumination and
standard g-line photoresist.
35Future LithographyPlasmon Lithography
- Atwater and co-workers from Caltech introduced
plasmon lithography in 2002. - Plasmon lithography is based on plasmon resonance
occurring in nanosized metallic structures,
allowing for the replication of patterns with a
resolution limit considerable below the
diffraction limit. - Is similar to ANSOM but with the scattering probe
tip is replaced by nanoparticles.
36Future LithographyBlock Copolymers
- Block copolymers comprise two or more different
monomer units, strung together in long sequences,
which can self-assemble into highly-ordered
lattices with unit cells dimensions of 10-100 nm.
This length scale reaches well below the limits
of conventional optical lithography. - Block copolymer lithography refers to the use of
block copolymers in the form of thin films in
which the domain structure provides a template
for additive or subtractive pattern transfer
operations.
37Future Lithography Zone plate array lithography
- Zone-Plate-Array Lithography (ZPAL), requires no
masks, but rather uses arrays of individually
targetable optical beams. - Beamlets of photons, which can be rapidly turned
on and off, are projected through diffractive
Fresnel-zone-plate lenses allowing myriad complex
shapes to be fabricated. - The zone plates are made using lithography
techniques and the shutters under each beamlet
are micromechanical. - ZPAL was originally developed at MITs
nanostructures laboratory in the mid to late
1990s. Each zoneplate is responsible for one unit
cell of photoresist exposure corresponding to the
diameter of a one individual zoneplate. The
writing with the shutters on and off results in a
dot-matrix type lines and moving the wafer in a
serpentine fashion under the focused beamlets
results in a full pattern.
38Future Lithography Zone plate array lithography
- Zone plates use constructive interference of
light rays from adjacent zones (Fresnel Zones) to
form a focus. The zones are spaced so that
diffracted-light constructively interferes at the
desired focus. The Fresnel zone plate is a
relative of the pinhole camera in that it does
not use mirrors or lenses for its imaging
properties. - The zone plate is especially useful in the
ultraviolet and x-ray regions of the spectrum,
for which other imaging devices are hard to find.
Self-supporting gold zone plates have been
manufactured for these spectral regions.
39 Future Lithography Quantum Lithography
- It has been demonstrated that quantum-lithography
with entangled N-photon states beats the Rayleigh
diffraction limit by a factor of N, and in
two-photon lithography the resolution is thus
improved by a factor of 2 (as if one used a
classical source with wavelength ?/2). - Einstein, Poldosky and Rosen described the
entangled two-particle state according to the
principle of quantum superposition in 1935 and
they pointed out a surprising consequence the
momentum ?Px (position ?x) for neither photon is
known - If one particle is measured to have a certain
momentum (position), the momentum (position) of
its twin is known with certainty, despite the
distance between them (this is known as the EPR
paradox). - The entangled photon pairs come out from a point
of the object plane, undergo two-photon
diffraction, and result in twice narrower point
spread function on the image plane.
40Future Lithography Superlens
- A poors man near-field superlens (e lt1 and m1)
was demonstrated. Zhang et al imaged objects as
small as 40-nm across with their superlens, which
is just 35-nm thick - This superlens images 10 nm features with 365 nm
light N. Fang, H. Lee, C. Sun, and X. Zhang,
Sub-diffraction-limited optical imaging with a
silver superlens, Science 308, 534-537 (2005). - Pendrys dream.
41Future LithographyStamp Lithography
- Soft lithography (Whitesides)
- Replication of a master-pattern using PDMS
(stamp) - Inking the stamp with molecules (thiols,
thioethers, alkoxysilanes, chlorosilanes, etc.) - Contact the stamp with the substrate surface
- Monolayer formation at regions of contact
42Future Lithography Nanoimprint Lithography
- Nanoimprint lithography (NIL) and Step-and-Flash
Imprint Lithography (SFIL) are techniques that
use hard molds instead of the soft molds used in
Soft Lithography. - Stephen Chou at Princeton University invented
nanoimprint lithography (NIL) in 1994, with the
aim of overcoming the diffraction limited minimal
feature sizes obtained in semiconductor
manufacturing based on DUV lithography
(http//www.princeton.edu/chouweb/).
43Future Lithography Nano-Imprint Technology (NIL)
- Nanoimprintlithography patterns a resist by
deforming the resist shape through embossing
(with a mold), rather than by altering resist
chemical structures through radiation (with
particle beams). After imprinting the resist, an
anisotropicetching is used to remove the residue
resist in the compressed area to expose the
underneath substrate. 10nm diameter holes and
40nm pitch in PMMA can be achieved on Si or a
metal substrate and excellent uniformity over 1
square inch.
44Future Lithography Nanoimprinting (NIL)
45Future LithographyStep-and-Flash Imprint
Lithography (SFIL)
- The University of Texas (UT)-Austin developed its
version of nanoimprint lithography, i.e.,
step-and-flash imprint lithography (SFIL), in
1998. - The SFIL method is distinct from the original NIL
in its use of UV-assisted nanoimprinting that
molds photocurable liquids in a step-and-repeat,
die-by-die fashion rather than by heat-assisted
molding of full, polymer-coated wafers.