Bio-microelectrical mechanical systems (BioMEMS) and Nanobiotechnology Dr. Shalini Prasad Electrical and Computer Engineering Biomedical Microdevices and Nanotechnology Laboratory sprasad@pdx.edu http://www.ece.pdx.edu/~prasads ECE 510 S. Prasad Slide:1 Courtesy: S.S. Saliterman Course Outline 1. Introduction to Bio-MEMS and Nanobiotechnology 2. Silicon Microfabrication 3. “Soft” Fabrication Techniques 4.Polymer Materials and Microfluidics 5. Sensor Principles 6.Detection and Measurement Methods 7. Drug delivery systems 8. Micro-Total Analysis Systems (μTAS)/ Emerging Applications 9. Nanotechnology Applications ECE 510 S. Prasad Slide:2 Courtesy: S.S. Saliterman Detection and Measurement Methods • Choosing a detection and measurement system for a specific application may depend on the preference for a labeled versus a label-free methodology • Some of the measurement systems are integral to the detection scheme such as confocal laser microscopy • Various measurement systems are also available for characterization of Si, glass and polymer materials post fabrication and/or surface modification ECE 510 S. Prasad Slide:3 Courtesy: S.S. Saliterman Detection and Measurement Methods • Profilometry, is an example of a surface measurement system • Most techniques are used for either detection or characterization • All need to be miniaturized or adapted for LOC and μTAS systems ECE 510 S. Prasad Slide:4 Courtesy: S.S. Saliterman Detection Methods ECE 510 S. Prasad Slide:5 Courtesy: S.S. Saliterman Electrochemical Detection (EC) • EC liquid analysis is associated with the measurement of electrical quantities such as potential, current and charge in order to gain information about the composition of the solution and the reaction kinetics of its components • EC is less expensive than fluorescent techniques • EC detection is suitable for LOC devices ECE 510 S. Prasad Slide:6 Courtesy: S.S. Saliterman Electrochemical Detection (EC) • Emerging technologies with EC detection incorporate micro fabrication of electrodes within the device as opposed to external electrodes • Capillary Electrophoresis devices were among the first to incorporate micro fabrication of integrated electrodes • Example- Baldwin’s work in Catechol detection ECE 510 S. Prasad Slide:7 Courtesy: S.S. Saliterman Electrochemical Detection Schemes ECE 510 S. Prasad Slide:8 Courtesy: S.S. Saliterman LOC device for Catechol Detection • Both CE channels and all the CE/EC electrodes were incorporated directly on to the glass substrates via traditional micro fabrication techniques- photolithographic patterning, wet chemical etching, DC sputtering and thermal wafer bonding • Critical electrode characteristics, including size, shape, and positions were fabricated into the chip eliminating the need for external electrodes. ECE 510 S. Prasad Slide:9 Courtesy: S.S. Saliterman LOC device for Catechol Detection • There are four CE reservoirs- sample, waste, buffer and detection • These are formed by drilling through the upper glass substrate • The corresponding Pt CE electrodes were patterned on to the bottom plates • Channels are 20-50 μm deep, 50-100 μm wide and 1-2 cm long. ECE 510 S. Prasad Slide:10 Courtesy: S.S. Saliterman LOC device for Catechol Detection • To achieve the 250 V/cm electric fields required for short-length CE tube, Baldwin et al used external power supply delivering 250 V and 2500 V DC for the injection and separation channels respectively. • EC detection is carried out amperometrically with a 3 electrode potentiostat constructed from Op-amps and passive elements ECE 510 S. Prasad Slide:11 Courtesy: S.S. Saliterman LOC device for Catechol Detection • The CE electrodes varying in thickness from 0.1-0.5 μm, 500 μm-1 mm in width and 1 cm in length. • Pt deposits placed in each of the reservoirs, located as far as possible from the CE channels • This is done to minimize the possibility that any form of electrolysis may disrupt flow in channel ECE 510 S. Prasad Slide:12 Courtesy: S.S. Saliterman LOC device for Catechol Detection • EC electrodes consist of Pt electrodes that are 0.1-0.5 μm thick and are placed only in the detection reservoir • The working and reference electrodes are 20-50 μm wide semicircular Pt fingers located at various positions on the chip • Catechols were separated at a detection sensitivity of μg/ml ECE 510 S. Prasad Slide:13 Courtesy: S.S. Saliterman Integrated CE and EC ECE 510 S. Prasad Slide:14 Courtesy: S.S. Saliterman Chemiluminescence ECE 510 S. Prasad Slide:15 Courtesy: S.S. Saliterman Chemiluminescence ECE 510 S. Prasad Slide:16 Courtesy: S.S. Saliterman Examples ECE 510 S. Prasad Slide:17 Courtesy: S.S. Saliterman Chemiluminescence Detection • Unlike, fluorescence where an excitation source is needed and non-specific radiation can be produced, CL occurs only when the reactants are present and noise is inherently low. • Detection of hybridizations using enzymecatalyzed CL reactions and micro glass array has been performed • A flow thru chip consisting pof 3D ordered set of micro channels and a micro array platform is fabricated • Analyte specific reagents or probes are deposited on the chip in an array of spots ECE 510 S. Prasad Slide:18 Courtesy: S.S. Saliterman Chemiluminescence Detection • Each spot incorporates several individual channel sand imaging is accomplished using a CCD camera • Rapid bacterial detection has also been demonstrated using this technique, bacteria is bound to a modified CL probe and quorum sensing based bioluminiscene is achieved ECE 510 S. Prasad Slide:19 Courtesy: S.S. Saliterman Chemiluminescence Detection ECE 510 S. Prasad Slide:20 Courtesy: S.S. Saliterman Fluorescence ECE 510 S. Prasad Slide:21 Courtesy: S.S. Saliterman Fluorescence • When illuminated at different wavelengths, some molecules emit light of a different color than the excitation wavelength. • The molecules absorb the higher energy wavelength, lose some energy in the form of lower energy photons. • Also known as red shift ECE 510 S. Prasad Slide:22 Courtesy: S.S. Saliterman Fluorescent Microscopy • It is shown schematically in the next viewgraph. • Excitation light is reflected off a dichoric mirror, through the objective lens on to t he sample • Dichromatic mirrors reflect light shorter than a certain wavelength and pas light longer than the wavelength • Fluorescence from the sample is collected by the objective lens and being of longer wavelength ( lower energy), passes back through the dichoric mirror to a detector ECE 510 S. Prasad Slide:23 Courtesy: S.S. Saliterman Fluorescent Microscopy • Epifluorescence involves illuminating the specimen from above while in transfluorescence the excitation light comes from below the sample • LOC laser devices allow on-chip excitation • Disposable integrated micro fluidic device with self aligned planar micro lenses, LED’s as excitation sources and photodiodes as detectors has been demonstrated ( Seo and Lee, 2004) ECE 510 S. Prasad Slide:24 Courtesy: S.S. Saliterman Fluorescent Microscopy ECE 510 S. Prasad Slide:25 Courtesy: S.S. Saliterman Confocal Microscopy • Confocal scanning microscopy has significant utility for high density detection such as in DNA micro arrays • In, regular fluorescence, the entire sample is illuminated by the excitation light causing the entire sample to fluoresce, therby creating a blurred image • The addition of a pinhole filters out light that is out-of-plane with the desired light ECE 510 S. Prasad Slide:26 Courtesy: S.S. Saliterman Confocal Microscopy • The object lens forms an image at the pinhole surface and the sample and the pinhole planes are called conjugate planes. • The pinhole is conjugate to the focal point of the lens thus the term confocal microscopy • As, in fluorescence microscopy light from the laser-higher wavelength light- is reflected by the dichoric mirror through the objective lens on to the sample ECE 510 S. Prasad Slide:27 Courtesy: S.S. Saliterman Confocal Microscopy • The fluorescence-lower wavelength-is gathered by the objective lens , passes through the dichoric mirror and is focused on to the pinhole surface • A photomultiplier tube measures fluorscent energy. • Moving mirrors allow the entire sample to be scanned ECE 510 S. Prasad Slide:28 Courtesy: S.S. Saliterman Multiple Exposure ECE 510 S. Prasad Slide:29 Courtesy: S.S. Saliterman Rotatory Confocal Fluorescence Scanner ECE 510 S. Prasad Slide:30 Courtesy: S.S. Saliterman Rotatory Confocal Fluorescence Scanner • The Berkley rotary confocal fluorescence scanner used to interrogate radial micro capillary array electrophoresis devices. • Laser excitation at 488 nm is reflected by a dichoric beamsplitter through a hollow shaft stepper motor and deflected 1.0 cm off axis by a rhomb prism mounted on the motor shaft. • Laser excitation is focused and fluorescence is collected by the microscope objective and reflected back through the beam splitter back to the detector ECE 510 S. Prasad Slide:31 Courtesy: S.S. Saliterman Rotatory Confocal Fluorescence Scanner • Fluorescence is spectrally filtered (dichoric beamsplitter and band pass filter), spatially filtered ( pinhole) and four color processed • Oosterbroek and van den Berg (2003) ECE 510 S. Prasad Slide:32 Courtesy: S.S. Saliterman Molecular Beacons ECE 510 S. Prasad Slide:33 Courtesy: S.S. Saliterman Molecular Beacons • The loop contains a probe sequence that is complementary to the target sequence • The stem, is formed by the annealing of complementary arm sequences that are locate don either side of the probe sequence • A fluorophore is covalently linked to the end of one arm and a quencher is linked covalently to the end of the other arm ECE 510 S. Prasad Slide:34 Courtesy: S.S. Saliterman Molecular Beacons • When MB’s hybridize to the appropriate target nuclei strands, the probe transitions from dark to fluorescence as the conformal changes move the fluorophore away from the non fluorescent quencher • This is known as fluorescence resonance energy transfer • When the probe encounters a target molecule it forms a probe target hybrid that iis longer and more stable than the stem hybrid • Ideal for genetic tests due to single nucleotide sensitivity ECE 510 S. Prasad Slide:35 Courtesy: S.S. Saliterman Molecular Beacons Applications ECE 510 S. Prasad Slide:36 Courtesy: S.S. Saliterman Aptamers ECE 510 S. Prasad Slide:37 Courtesy: S.S. Saliterman Example: Thrombin Aptamer ECE 510 S. Prasad Slide:38 Courtesy: S.S. Saliterman Characterization ECE 510 S. Prasad Slide:39 Courtesy: S.S. Saliterman Interferometry ECE 510 S. Prasad Slide:40 Courtesy: S.S. Saliterman Interference • Interferometers utilize the physical phenomenon of interference patterns • Interference occurs with the superposition of two or more EM waves • For coherent visible light with similar frequency and phase and travelling in the same direcytion this may be observed as fringes of dark and light, which are based on addition and subtraction of wave components at a given point. • These are referred to as maxima and minima ECE 510 S. Prasad Slide:41 Courtesy: S.S. Saliterman Diffraction • Diffraction occurs whenever a wavefront is obstructed such as passing through a single slit with resulting alteration of amplitude and phase • Fringes or diffraction patterns are formed as some EM radiation bends around the obstacle unto the shadow and mutually interfere ECE 510 S. Prasad Slide:42 Courtesy: S.S. Saliterman Interferometry Interference fringes by splitting a beam of monochromatic light so that one beam strikes the foxed mirror and the other the movable mirror The beams are reflected back to the common target producing interference patterns S. Prasad Slide:43 ECE 510 Courtesy: S.S. Saliterman Interferometry • Interference based integrated optical sensors such as Mach-Zehnder interferometer can detect refractive index changes as small as 10-8, this corresponds to protein concentrations of 5.3x10-8 g/ml. ECE 510 S. Prasad Slide:44 Courtesy: S.S. Saliterman Ellipsometry • Ellipsometry is used to measure optical and surface properties of materials and thin films • In plane polarized EM radiation all electronic oscillations are parallel to each other and at right angles to the magnetic oscilklations • Light can be plane polarized by reflection or passing through polaroid filter ECE 510 S. Prasad Slide:45 Courtesy: S.S. Saliterman Ellipsometry • In an ellipsometer laser light is produced at the source and retarders shift the phase of one component of the incident light . • If a light beam illuminates a thin film/substrate surface under oblique incidence, reflection from the surface changes the ellipse of polarization ECE 510 S. Prasad Slide:46 Courtesy: S.S. Saliterman Ellipsometry ECE 510 S. Prasad Slide:47 Courtesy: S.S. Saliterman Surface Plasmon Resonance (SPR) Spectroscopy • SPR measurements are made using optical systems that control the angle and wavelength of incident light and the degree of polarization • This technique is commonly used to study ultra thin films with immobilized bio molecules • A combination of substrate, noble metal and sample allows for the generation of surface plasmon polaritons ECE 510 S. Prasad Slide:48 Courtesy: S.S. Saliterman Surface Plasmon Resonance (SPR) Spectroscopy • These are formed along the metal dielectric interface and are highly damped charge density waves that oscillate at optical frequencies and may be excited if the materials and optical properties of the experimental systems are properly chosen. • SPPs are not measured directly but their presence is inferred by monitoring the light intensity reflected from substrate/metal interface • The reflected light contains a deep minimum in intensity at what is termed as resonance for the surface plasmon. ECE 510 S. Prasad Slide:49 Courtesy: S.S. Saliterman Surface Plasmon Resonance ECE 510 S. Prasad Slide:50 Courtesy: S.S. Saliterman Raman Microscopy ECE 510 S. Prasad Slide:51 Courtesy: S.S. Saliterman Raman Microscopy ECE 510 S. Prasad Slide:52 Courtesy: S.S. Saliterman Electron Microscopy • Electron microscopes use a focused beam of electrons for imaging rather than light • Scanning electron microscopes use “scanning” beam of electrons across the sample making it possible to study, topology, morphology, composition and crystallographic qualities of the materials • Topology includes surface features, texture from which properties such as reflectivity and hardness may be inferred ECE 510 S. Prasad Slide:53 Courtesy: S.S. Saliterman Electron Microscopy • Morphology is the shape and size of the particles making up the object from which properties such as ductility, strength and reactivity may be inferred • Composition includes the elements and compounds that compose an object and the relative abundance of their existence that affect properties such as melting point, hardness and reactivity. ECE 510 S. Prasad Slide:54 Courtesy: S.S. Saliterman Electron Microscopy • TEM is the primary tool for observation of crystal defects including dislocations, grain boundaries, interphase interfaces and other planar defects • TEM may be coupled with x-ray detectors and electron spectrometers allowing quantitative analysis of all the elemnts in the samoke with sensitivity upto single antom levels ECE 510 S. Prasad Slide:55 Courtesy: S.S. Saliterman Electron Microscopy ECE 510 S. Prasad Slide:56 Courtesy: S.S. Saliterman Electron Microscopy ECE 510 S. Prasad Slide:57 Courtesy: S.S. Saliterman Atomic Force Microscopy • Is a form of scanned proximity probe microscope in which measuring a local property such as height, optical absorption, or magnetism is performed by placing a probe near the sample • The probe sample separations are on the order of system resolution and imaging occurs by raster scanning the surface of interest • AFM measures topography with a force probe, and operates by measuring the attractive or repulsive force between the probe tip and the sample ECE 510 S. Prasad Slide:58 Courtesy: S.S. Saliterman Atomic Force Microscopy • In contact mode a cantilever tip lightly touches the sample while deflection of the cantilever is measured and related to height • Measuring cantilever deflection with the angular deflection of the laser beam allows picometer resolution • In non contact mode the tip does not touch the sample but instead measures the attractive forces. ECE 510 S. Prasad Slide:59 Courtesy: S.S. Saliterman Atomic Force Microscopy ECE 510 S. Prasad Slide:60 Courtesy: S.S. Saliterman Summary ECE 510 S. Prasad Slide:61 Courtesy: S.S. Saliterman