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Title: Photolithography, Next Generation Lithography and Future Lithography 5b


1
Photolithography, Next Generation Lithography and
Future Lithography (5b)
  • Winter 2009

2
Next 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)
4
Next Generation Lithography (NGL)
5
Next 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

6
Next Generation Lithography EUV
  • Mask fabrication is the most difficult task

7
Next 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.

8
Next 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

9
Next 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

10
Next Generation Lithography E-Beam
11
Next 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

12
Next Generation Lithography E-Beam
  • E-beam blur

13
Next 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

14
Next Generation LithographyE-Beam
15
Next 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

16
Next 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)
18
Next 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
19
Next 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

20
Next 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

21
Next 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.

22
Next 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

23
Next 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.

24
Next Generation LithographyIPL
  • IPL Mask

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).

26
Future 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.

27
Future 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.

28
Future 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.

29
Future 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

30
Future 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.

31
Future 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.

32
Future 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.

33
Future 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.

34
Future 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.

35
Future 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.

36
Future 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.

37
Future 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.

38
Future 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.

40
Future 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.

41
Future 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

42
Future 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/).

43
Future 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.

44
Future Lithography Nanoimprinting (NIL)
45
Future 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.
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