Microwave
  Filter

 Microwave Engineering
       CHO, Yong Heui
Microwave Engineering




Circuit Resonator

        2           EM Wave Lab
Microwave Engineering
1. LC resonator

Applications

    
     
         Filter
         Oscillator
        Frequency meter
        Tuned amplifier




                           3          EM Wave Lab
Microwave Engineering
1. LC resonator

LC resonator: ideal resonator

     Input impedance
                         j
           Z in = jωL −
                        ωC
      Input power
               1 * 1       2 1 2        j 
          Pin = VI = Z in I = I  jωL −    
               2    2        2         ωC 
      Resonant frequency: Wm = We
                  1
          ω=
                  LC

                             4               EM Wave Lab
Microwave Engineering
1. LC resonator

Series resonator

     R, L, C
      Input impedance
                           j
         Z in = R + jωL −
                          ωC
      Input power
              1 * 1       2 1 2            j 
         Pin = VI = Z in I = I  R + jωL −    
              2    2        2             ωC 
      Resonant frequency
                  1
          ω=
                  LC
                               5             EM Wave Lab
Microwave Engineering
1. LC resonator

Quality factor

     Definition
              Average energe stored
         Q =ω
               Energy loss/second
      3 dB bandwidth
                f0
            Q=
               BW
      Q in terms of R, L, C
                 2Wm ω 0 L      1
          Q = ω0     =     =
                  Pl   R     ω 0 RC
                               6             EM Wave Lab
Microwave Engineering
1. LC resonator

Perturbation

     Input impedance
                         ω 2 − ω0 
                                 2
          Z in = R + jωL
                         ω 2  ≈ R + j 2 L∆ω
                                   
                                  




                           7                    EM Wave Lab
Microwave Engineering
1. LC resonator

Parallel resonator

     R, L, C
      Input admittance
              1  j
         Yin = −   + j ωC
              R ωL
      Input power
             1 * 1 * 2 1 2 1     j        
        Pin = VI = Yin V = V  +    − j ωC 
             2    2       2   R ωL        
      Resonant frequency
                  1
          ω=
                  LC
                            8              EM Wave Lab
Microwave Engineering
1. LC resonator

Quality factor

     Q in terms of R, L, C
                2Wm    R
         Q = ω0     =      = ω 0 RC
                 Pl   ω0 L




                               9             EM Wave Lab
Microwave Engineering
1. LC resonator

Perturbation

     Input admittance
              1       ω 2 − ω0  1
                              2
         Yin = + jωC 
                      ω 2  ≈ R + j 2C∆ω
                                
              R                




                          10                EM Wave Lab
Microwave Engineering
1. LC resonator

Loaded Q

     Unloaded Q: resonant circuit itself
      Loaded Q: External load resistor
            1   1 1
              =  +
            QL Qe Q




                             11                     EM Wave Lab
Microwave Engineering
2. Tx line resonator

 Short-circuited half-wave line

     Transmission line
      Input impedance: lossy medium
            Z in = Z 0 tanh (α + jβ ) l
                  tanh(αl ) + j tan( βl )
            = Z0
                 1 + j tan( βl ) tanh(αl )




                                  12                EM Wave Lab
Microwave Engineering
2. Tx line resonator

 Approximation

     Low-loss transmission line
         tanh(αl ) ≈ αl
      Phase: ω = ω 0 + ∆ω , l = λ / 2
                           ∆ωπ     ∆ωπ
       tan( βl ) = tan(π +     )≈
                            ω0      ω0




                           13                   EM Wave Lab
Microwave Engineering
2. Tx line resonator

 Equivalence

     Input impedance
                  αl + j (∆ωπ / ω 0 )               ∆ωπ   
       Z in ≈ Z 0                      ≈ Z 0 αl + j
                                                          
                                                           
                  1 + j (∆ωπ / ω 0 )αl               ω0   
       = R + 2 jL∆ω
      Quality factor
              ω0 L π     β
           Q=     =    =
               R    2αl 2α


                               14                      EM Wave Lab
Microwave Engineering
2. Tx line resonator

 Open-circuited half-wave line

     Transmission line
      Input impedance: lossy medium
            Z in = Z 0 coth (α + jβ ) l
                 1 + j tan( βl ) tanh(αl )
            = Z0
                  tanh(αl ) + j tan( βl )




                                  15                EM Wave Lab
Microwave Engineering
2. Tx line resonator

 Approximation

     Low-loss transmission line
         tanh(αl ) ≈ αl
      Phase: ω = ω 0 + ∆ω , l = λ / 2
                           ∆ωπ     ∆ωπ
       tan( βl ) = tan(π +     )≈
                            ω0      ω0




                           16                   EM Wave Lab
Microwave Engineering
2. Tx line resonator

 Equivalence

     Input impedance
                  1 + j (∆ωπ / ω 0 )αl        Z0
       Z in ≈ Z 0                      ≈
                  αl + j (∆ωπ / ω 0 ) αl + j (∆ωπ / ω 0 )
                 1
       =
         1 / R + 2 jC∆ω
      Quality factor
                        π   β
          Q = ω 0 RC =    =
                       2αl 2α

                              17                       EM Wave Lab
Microwave Engineering
3. Waveguide cavity

Rectangular waveguide

     Metallic wall
      Propagation constant
                            2        2
                      mπ   nπ 
         β mn   = k −2
                           −   
                      a   b 
      Resonant condition
          β mn d = lπ



                            18                  EM Wave Lab
Microwave Engineering
3. Waveguide cavity

Resonant wavenumber

     Resonant wavenumber
                       2          2       2
                  mπ   n π   l π 
       k mnl   =      +     + 
                  a   b  d 
      TE101 mode and TM110 mode
      Q of cavity
                      2We
               Q = ω0
                       Pl


                             19                      EM Wave Lab
Microwave Engineering
3. Waveguide cavity

Circular waveguide

     Metallic wall
      Propagation constant
      Resonant condition
          β mn d = lπ
      TE111 mode and TM110 mode




                          20              EM Wave Lab
Microwave Engineering
4. Dielectric cavity

 Dielectric material

     
      
          High Q
          Fringing field
         High permittivity: magnetic wall
         Mechanical tuning
         TE01δ mode
         Notation
           δ = 2 L / λg < 1




                               21                   EM Wave Lab
Microwave Engineering
5. Mirror

 Fabry-Perot resonator

     
      
            Two mirrors
            High Q
           Laser
           Millimeter and optical applications




                                 22                      EM Wave Lab
Microwave Engineering




Microwave Filter

        23          EM Wave Lab
Microwave Engineering
1. Filter

 Characteristics

     2 port network: S parameters
      Pass band and stop band
      Return loss and insertion loss
      Ripple and selectivity (skirt)
      Pole and zero
      Group delay




                             24                EM Wave Lab
Microwave Engineering
1. Filter

 Characteristics

        Phase response
         Signal distortion




                              25          EM Wave Lab
Microwave Engineering
1. Filter

 Classification

     
      
            LPF (Low Pass Filter)
            HPF (High Pass Filter)
           BPF (Band Pass Filter)
           BSF (Band Stop Filter): notch filter




                                  26                      EM Wave Lab
Microwave Engineering
1. Filter

 Filter response

     
      
            Maximally flat (Butterworth) filter
            Chebyshev filter
           Elliptic function filter
           Bessel function filter




                                  27                     EM Wave Lab
Microwave Engineering
2. Filter design

 Design process

     
      
          Filter specifications
          Design of low pass filter
         Scaling and conversion
         Design of transmission line
         Implementation




                              28               EM Wave Lab
Microwave Engineering
2. Filter design

 Insertion loss method

      Precise design method
       Power loss ratio: transducer gain
              Power available from source        1
        PLR =                             =           2
                Power delivered to load     1 − Γ(ω )
       Reflection coefficient
                  2        M (ω 2 )
             Γ(ω ) =
                      M (ω 2 ) + N (ω 2 )
       Results:            M (ω 2 )
                  PLR = 1 +
                            N (ω 2 )
                              29                    EM Wave Lab
Microwave Engineering
2. Filter design

 Filter responses: LPF

       Maximally flat response
                                         2N
                                ω 
                    PLR = 1 + k  
                                 2
                                ω 
                                 c
        Equal ripple response
                                 ω 
                   PLR = 1 + k T  
                                 2
                                 ω 
                                     2
                                     N
                                  c
        Chebyshev polynomial
                   TN (cosθ ) = cos(nθ )

                            30                       EM Wave Lab
Microwave Engineering
2. Filter design

 Example

      Design 2-poles low pass filter in terms of the
        insertion loss method where ω c = 1, Z S = 1


                      PLR = 1 + ω 4

                            Z L (1 − jωZ L C )
               Z in = jωL +
                             1 + (ωZ L C ) 2




                                31                      EM Wave Lab
Microwave Engineering
2. Filter design

 Impedance scaling

                                   Z L (1 − jωZ L C )
       L′ = Z 0 L    Z in = jωL +
                                    1 + (ωZ L C ) 2

             C
        C′ =                     Example
             Z0                    ω0 L
                                Q=
         ′
        Zs = Z0                     R
          ′
        Z L = Z0Z L                    1
                               ω0 =
                                       LC
                           Series RLC resonator

                          32                       EM Wave Lab
Microwave Engineering
2. Filter design

 Frequency scaling for LPF

      Basic equation
                              ω 
               PLR (ω ) = PLR  
                ′             ω 
                               c

             ω                              L
      jX = j    L = j ωL ′            L′ =
             ωc                             ωc
             ω                              C
      jB = j C = jωC ′                 C′ =
             ωc                             ωc

                              33                        EM Wave Lab
Microwave Engineering
2. Filter design

 Frequency scaling for HPF

      Basic equation
                              ωc 
               ′
              PLR (ω ) = PLR  − 
                              ω 

              ωc       1                     1
     jX = − j    L=                   L′ =
              ω     j ωC ′                  ω cC
              ωc      1                      1
     jB = − j C =                      C′ =
              ω     j ωL ′                  ωc L

                              34                          EM Wave Lab
Microwave Engineering
2. Filter design

 Frequency scaling for BPF

      Basic equation:    ω 0 = ω1ω 2
                           ω ω0  
           ′              Q
          PLR (ω ) = PLR      −    , Q = ω 0
                            ω0 ω  
                                            ω 2 − ω1

                 ω ω0                 1
        jX = jQ
                 ω − ω  L = jωL1′ − jωC ′
                        
                 0                      1

                 ω ω0                 1
         jB = jQ
                ω  − C = jωC2 − ′
                 0   ω 
                                      jωL2′

                              35                      EM Wave Lab
Microwave Engineering
2. Filter design

 Frequency scaling for BSF

      Basic equation:    ω 0 = ω1ω 2
                         1 ω   ω  
                                      −1

          ′
         PLR (ω ) = PLR   0 −  , Q = ω 0
                         Q  ω ω0  
                                      ω 2 − ω1
                        
                          −1                          −1
            j  ω0 ω                 1          
       jX =  −  L =                ωL′ − ωC1′ 
                                    j            
            Q  ω ω0 
                                    1          
                          −1                          −1
            j  ω0 ω                 1          
        jB =     −  C=            j          ′
                                      ωC ′ − ωL2 
            Q  ω ω0 
                                    2          
                               36                          EM Wave Lab
Microwave Engineering
2. Filter design

 Example

      Design 5-poles low pass filter with a cutoff
        frequency of 2 [GHz], impedance = 50 [Ohms],
        insertion loss = 15 dB at 3 [GHz]
        g1 = 0.618
        g 2 = 1.618
        g3 = 2
        g 4 = 1.618
        g 5 = 0.618
   Maximally flat response

                             37                    EM Wave Lab
Microwave Engineering
2. Filter design

 Richard’s transformation

      Transformation
                                ωl 
            Ω = tan( βl ) = tan 
                               v 
                                p
       Input impedance: stub

            jX = jΩL = jL tan( βl )
            jB = jΩC = jC tan( βl )




                               38              EM Wave Lab
Microwave Engineering
2. Filter design

 LC to stubs




                  jX = jΩL = jL tan( βl )




                  jB = jΩC = jC tan( βl )
                              39                    EM Wave Lab
Microwave Engineering
2. Filter design

 Stub characteristics

      Resonance: wavelength/8 related to the cutoff
        frequency
                   Ω = 1 = tan( βl )
       Attenuation pole: wavelength/4

       Period: wavelength/2




                               40                   EM Wave Lab
Microwave Engineering
2. Filter design

 Kuroda’s identity

      Stub transformation: shunt and series stub

       Series to shunt stub transform: microstrip line
                           Z2
                    N = 1+
                           Z1
       Implementation




                              41                     EM Wave Lab
Microwave Engineering
2. Filter design

 Kuroda’s identity




                          
                          Stub transformation


                     42                EM Wave Lab
Microwave Engineering
2. Filter design

 Equivalent transmission line

      Series to shunt stub transform: microstrip line
       Implementation: realization




                              43                     EM Wave Lab
Microwave Engineering
3. Implementation

Materials

    
     
         Microstrip line
         Dielectric resonator
        Waveguide
        Semiconductor
        MEMS (Micro ElectroMechanical System)
        LTCC (Low Temperature Cofired Ceramic)
        SAW (Surface Acoustic Wave)
        FBAR (Film Bulk Acoustic Resonator)
        Superconductor




                            44                    EM Wave Lab

Microwave Filter

  • 1.
    Microwave Filter Microwave Engineering CHO, Yong Heui
  • 2.
  • 3.
    Microwave Engineering 1. LCresonator Applications    Filter Oscillator  Frequency meter  Tuned amplifier 3 EM Wave Lab
  • 4.
    Microwave Engineering 1. LCresonator LC resonator: ideal resonator   Input impedance j Z in = jωL − ωC  Input power 1 * 1 2 1 2 j  Pin = VI = Z in I = I  jωL −  2 2 2  ωC   Resonant frequency: Wm = We 1 ω= LC 4 EM Wave Lab
  • 5.
    Microwave Engineering 1. LCresonator Series resonator   R, L, C  Input impedance j Z in = R + jωL − ωC  Input power 1 * 1 2 1 2 j  Pin = VI = Z in I = I  R + jωL −  2 2 2  ωC   Resonant frequency 1 ω= LC 5 EM Wave Lab
  • 6.
    Microwave Engineering 1. LCresonator Quality factor   Definition Average energe stored Q =ω Energy loss/second  3 dB bandwidth f0 Q= BW  Q in terms of R, L, C 2Wm ω 0 L 1 Q = ω0 = = Pl R ω 0 RC 6 EM Wave Lab
  • 7.
    Microwave Engineering 1. LCresonator Perturbation   Input impedance  ω 2 − ω0  2 Z in = R + jωL  ω 2  ≈ R + j 2 L∆ω    7 EM Wave Lab
  • 8.
    Microwave Engineering 1. LCresonator Parallel resonator   R, L, C  Input admittance 1 j Yin = − + j ωC R ωL  Input power 1 * 1 * 2 1 2 1 j  Pin = VI = Yin V = V  + − j ωC  2 2 2  R ωL   Resonant frequency 1 ω= LC 8 EM Wave Lab
  • 9.
    Microwave Engineering 1. LCresonator Quality factor   Q in terms of R, L, C 2Wm R Q = ω0 = = ω 0 RC Pl ω0 L 9 EM Wave Lab
  • 10.
    Microwave Engineering 1. LCresonator Perturbation   Input admittance 1  ω 2 − ω0  1 2 Yin = + jωC   ω 2  ≈ R + j 2C∆ω  R   10 EM Wave Lab
  • 11.
    Microwave Engineering 1. LCresonator Loaded Q   Unloaded Q: resonant circuit itself  Loaded Q: External load resistor 1 1 1 = + QL Qe Q 11 EM Wave Lab
  • 12.
    Microwave Engineering 2. Txline resonator Short-circuited half-wave line   Transmission line  Input impedance: lossy medium Z in = Z 0 tanh (α + jβ ) l tanh(αl ) + j tan( βl ) = Z0 1 + j tan( βl ) tanh(αl ) 12 EM Wave Lab
  • 13.
    Microwave Engineering 2. Txline resonator Approximation   Low-loss transmission line tanh(αl ) ≈ αl  Phase: ω = ω 0 + ∆ω , l = λ / 2 ∆ωπ ∆ωπ tan( βl ) = tan(π + )≈ ω0 ω0 13 EM Wave Lab
  • 14.
    Microwave Engineering 2. Txline resonator Equivalence   Input impedance αl + j (∆ωπ / ω 0 )  ∆ωπ  Z in ≈ Z 0 ≈ Z 0 αl + j    1 + j (∆ωπ / ω 0 )αl  ω0  = R + 2 jL∆ω  Quality factor ω0 L π β Q= = = R 2αl 2α 14 EM Wave Lab
  • 15.
    Microwave Engineering 2. Txline resonator Open-circuited half-wave line   Transmission line  Input impedance: lossy medium Z in = Z 0 coth (α + jβ ) l 1 + j tan( βl ) tanh(αl ) = Z0 tanh(αl ) + j tan( βl ) 15 EM Wave Lab
  • 16.
    Microwave Engineering 2. Txline resonator Approximation   Low-loss transmission line tanh(αl ) ≈ αl  Phase: ω = ω 0 + ∆ω , l = λ / 2 ∆ωπ ∆ωπ tan( βl ) = tan(π + )≈ ω0 ω0 16 EM Wave Lab
  • 17.
    Microwave Engineering 2. Txline resonator Equivalence   Input impedance 1 + j (∆ωπ / ω 0 )αl Z0 Z in ≈ Z 0 ≈ αl + j (∆ωπ / ω 0 ) αl + j (∆ωπ / ω 0 ) 1 = 1 / R + 2 jC∆ω  Quality factor π β Q = ω 0 RC = = 2αl 2α 17 EM Wave Lab
  • 18.
    Microwave Engineering 3. Waveguidecavity Rectangular waveguide   Metallic wall  Propagation constant 2 2  mπ   nπ  β mn = k −2  −   a   b   Resonant condition β mn d = lπ 18 EM Wave Lab
  • 19.
    Microwave Engineering 3. Waveguidecavity Resonant wavenumber   Resonant wavenumber 2 2 2  mπ   n π   l π  k mnl =   +  +   a   b  d   TE101 mode and TM110 mode  Q of cavity 2We Q = ω0 Pl 19 EM Wave Lab
  • 20.
    Microwave Engineering 3. Waveguidecavity Circular waveguide   Metallic wall  Propagation constant  Resonant condition β mn d = lπ  TE111 mode and TM110 mode 20 EM Wave Lab
  • 21.
    Microwave Engineering 4. Dielectriccavity Dielectric material    High Q Fringing field  High permittivity: magnetic wall  Mechanical tuning  TE01δ mode  Notation δ = 2 L / λg < 1 21 EM Wave Lab
  • 22.
    Microwave Engineering 5. Mirror Fabry-Perot resonator    Two mirrors High Q  Laser  Millimeter and optical applications 22 EM Wave Lab
  • 23.
  • 24.
    Microwave Engineering 1. Filter Characteristics  2 port network: S parameters Pass band and stop band Return loss and insertion loss Ripple and selectivity (skirt) Pole and zero Group delay 24 EM Wave Lab
  • 25.
    Microwave Engineering 1. Filter Characteristics   Phase response  Signal distortion 25 EM Wave Lab
  • 26.
    Microwave Engineering 1. Filter Classification    LPF (Low Pass Filter) HPF (High Pass Filter)  BPF (Band Pass Filter)  BSF (Band Stop Filter): notch filter 26 EM Wave Lab
  • 27.
    Microwave Engineering 1. Filter Filter response    Maximally flat (Butterworth) filter Chebyshev filter  Elliptic function filter  Bessel function filter 27 EM Wave Lab
  • 28.
    Microwave Engineering 2. Filterdesign Design process    Filter specifications Design of low pass filter  Scaling and conversion  Design of transmission line  Implementation 28 EM Wave Lab
  • 29.
    Microwave Engineering 2. Filterdesign Insertion loss method   Precise design method  Power loss ratio: transducer gain Power available from source 1 PLR = = 2 Power delivered to load 1 − Γ(ω )  Reflection coefficient 2 M (ω 2 ) Γ(ω ) = M (ω 2 ) + N (ω 2 )  Results: M (ω 2 ) PLR = 1 + N (ω 2 ) 29 EM Wave Lab
  • 30.
    Microwave Engineering 2. Filterdesign Filter responses: LPF   Maximally flat response 2N ω  PLR = 1 + k   2 ω   c  Equal ripple response ω  PLR = 1 + k T   2 ω  2 N  c  Chebyshev polynomial TN (cosθ ) = cos(nθ ) 30 EM Wave Lab
  • 31.
    Microwave Engineering 2. Filterdesign Example   Design 2-poles low pass filter in terms of the insertion loss method where ω c = 1, Z S = 1 PLR = 1 + ω 4 Z L (1 − jωZ L C ) Z in = jωL + 1 + (ωZ L C ) 2 31 EM Wave Lab
  • 32.
    Microwave Engineering 2. Filterdesign Impedance scaling Z L (1 − jωZ L C )  L′ = Z 0 L Z in = jωL + 1 + (ωZ L C ) 2 C C′ = Example Z0 ω0 L Q= ′ Zs = Z0 R ′ Z L = Z0Z L 1 ω0 = LC Series RLC resonator 32 EM Wave Lab
  • 33.
    Microwave Engineering 2. Filterdesign Frequency scaling for LPF   Basic equation ω  PLR (ω ) = PLR   ′ ω   c ω L jX = j L = j ωL ′  L′ = ωc ωc ω C jB = j C = jωC ′ C′ = ωc ωc 33 EM Wave Lab
  • 34.
    Microwave Engineering 2. Filterdesign Frequency scaling for HPF   Basic equation  ωc  ′ PLR (ω ) = PLR  −   ω  ωc 1 1 jX = − j L=  L′ = ω j ωC ′ ω cC ωc 1 1 jB = − j C = C′ = ω j ωL ′ ωc L 34 EM Wave Lab
  • 35.
    Microwave Engineering 2. Filterdesign Frequency scaling for BPF   Basic equation: ω 0 = ω1ω 2   ω ω0   ′  Q PLR (ω ) = PLR   −  , Q = ω 0   ω0 ω    ω 2 − ω1  ω ω0  1  jX = jQ  ω − ω  L = jωL1′ − jωC ′   0  1  ω ω0  1 jB = jQ ω − C = jωC2 − ′  0 ω   jωL2′ 35 EM Wave Lab
  • 36.
    Microwave Engineering 2. Filterdesign Frequency scaling for BSF   Basic equation: ω 0 = ω1ω 2  1 ω ω   −1 ′ PLR (ω ) = PLR   0 −  , Q = ω 0  Q  ω ω0      ω 2 − ω1  −1 −1 j  ω0 ω   1   jX =  −  L =  ωL′ − ωC1′  j  Q  ω ω0     1  −1 −1 j  ω0 ω   1  jB =  −  C= j ′  ωC ′ − ωL2  Q  ω ω0     2  36 EM Wave Lab
  • 37.
    Microwave Engineering 2. Filterdesign Example   Design 5-poles low pass filter with a cutoff frequency of 2 [GHz], impedance = 50 [Ohms], insertion loss = 15 dB at 3 [GHz] g1 = 0.618 g 2 = 1.618 g3 = 2 g 4 = 1.618 g 5 = 0.618 Maximally flat response 37 EM Wave Lab
  • 38.
    Microwave Engineering 2. Filterdesign Richard’s transformation   Transformation  ωl  Ω = tan( βl ) = tan  v   p  Input impedance: stub jX = jΩL = jL tan( βl ) jB = jΩC = jC tan( βl ) 38 EM Wave Lab
  • 39.
    Microwave Engineering 2. Filterdesign LC to stubs  jX = jΩL = jL tan( βl )  jB = jΩC = jC tan( βl ) 39 EM Wave Lab
  • 40.
    Microwave Engineering 2. Filterdesign Stub characteristics   Resonance: wavelength/8 related to the cutoff frequency Ω = 1 = tan( βl )  Attenuation pole: wavelength/4  Period: wavelength/2 40 EM Wave Lab
  • 41.
    Microwave Engineering 2. Filterdesign Kuroda’s identity   Stub transformation: shunt and series stub  Series to shunt stub transform: microstrip line Z2 N = 1+ Z1  Implementation 41 EM Wave Lab
  • 42.
    Microwave Engineering 2. Filterdesign Kuroda’s identity  Stub transformation 42 EM Wave Lab
  • 43.
    Microwave Engineering 2. Filterdesign Equivalent transmission line   Series to shunt stub transform: microstrip line  Implementation: realization 43 EM Wave Lab
  • 44.
    Microwave Engineering 3. Implementation Materials    Microstrip line Dielectric resonator  Waveguide  Semiconductor  MEMS (Micro ElectroMechanical System)  LTCC (Low Temperature Cofired Ceramic)  SAW (Surface Acoustic Wave)  FBAR (Film Bulk Acoustic Resonator)  Superconductor 44 EM Wave Lab