fig5 shows a longitudinal cross - sectional view of a portion of a shield tape &# 39 ; s overlap region ( a ). the shield tape &# 39 ; s longitudinal impedance has essentially two components ; a spiral resistive / inductive component and a capacitive component that arises from the tape &# 39 ; s overlap region . the overlap capacitance is controlled by the substrate thickness and the overlap width and length . in order to decrease the shield resonance magnitude and / or to increase the resonant frequency , some methods can be applied . in order to shift the resonant frequency up to higher frequencies , the over - lap to over - lap distance can be decreased . this is accomplished by having more wraps per unit length . to decrease the magnitude of the resonant spike , the overlap capacitance can be increased . one simple method of raising the capacitance ( and hence lowering the impedance ) is to decrease the tape &# 39 ; s substrate thickness and / or increase the overlap length ( as shown in fig5 a ). raising the capacitance lowers the longitudinal impedance and increases the amount of current that follows the em wave longitudinally down the cable . another technique is to use double metallic sided shield tape ( metal on both sides of a substrate ), which increases the capacitance as well . another way of decreasing the magnitude of the shield resonance peak is to break up and / or alter the periodicity of the overlap regions ( and hence reduce the in - phase constructive interference terms ). in fig5 b , a constant overlap to overlap periodicity is shown ( where at each of the overlap regions a reflection occurs that constructively interfere with each other at the cables endpoints and form a resonant response ), in fig5 c a random overlap length as a function of longitudinal length is shown ( which will break up the constructively adding interference waves , thereby reducing and broadening the resonant peak ) and fig5 d shows a sinusoidal varying overlap length . in c or d , the length between overlap to overlap periodicity is varied and the resonant peak is decreased accordingly . one way to implement a random or periodic overlap is to modulate ( or dither ) the tape application mechanism either longitudinally or tangential to the cable . another way to implement either a random or any periodic pattern to produce a longitudinally varying overlap is to use a metallic shield tape whose width has the random width or periodic width . fig6 a - 6e illustrate a proposed technique for reducing the shield resonance as well as improving the connection from the cable to the connector . if the shield tape overlap region can be effectively “ short - circuited ”, the magnitude of the resonance is reduced . this particular technique includes double wrapping shield tapes 104 a , 104 b around the wire - pair 102 ( shown in fig6 a and 6b ). the two tapes 104 a , 104 b can include a thin sheet of aluminum metal or other conductive material laminated upon an insulating substrate and have their metallic faces ( crosshatched surfaces in fig6 b and 6c ) towards each other , which may eliminate the need for a drain wire . in this technique , the shield wraps 104 a , 104 b can have the same widths as shown in fig6 a - 6b , or different widths ( fig6 c ), and wound in alternative directions which improves the conductivity between the shield tapes 104 a , 104 b and hence minimizes the shield resonant magnitude . the longitudinal cross - sectional view shown in fig6 d , describes how the two shield tapes 104 a , 104 b connect / conduct between them , as well as how the cable can be connected to a connector via crimp ferrules 122 , 124 . the cross - sectional front view is shown in fig6 e . although fig6 b and 6c show a drain wire 105 which typically may be used as a signal ground or reference and is typically electrically conductive with tapes 104 a , 104 b , drain wire 105 may not be needed when using a pair manager as described below . fig7 a shows a longitudinal cross sectional view of a twinax cable wire - pair 102 and a proposed connector interface to it . in fig7 a , an outer crimp ferrule 122 ( an example of which is shown in more detail in fig7 c ) is used to create a force acting on the outer shield 104 b and to the inner crimp / support ferrule 124 ( an example of which is shown in more detail in fig7 b ) so that the outer shield 104 b and the inner crimp / support ferrule 124 make a very low ( 360 °) electrical resistive connection . the other end of the inner crimp / support 124 ferrule is used to make contact to the connector &# 39 ; s circuit board 120 and keeping the impedance of the twinax cable wire - pair 102 as close to 100 ohm as possible . a “ pair - manager ” ( at least ferrule 124 , but can also include ferrule 122 ) is shown in fig7 a with at least a purpose of maintaining the characteristic impedance of the cable as it enters into the connector and to assist in mechanically aligning the twinax cable wire - pair 102 to the circuit board 120 . an example of the connector and circuit board 120 can be a sfp + connector as shown in u . s . patent application ser . no . 12 / 487 , 778 ( patel et al . ), filed jun . 19 , 2009 , incorporated by reference as if fully set forth herein . however , the present invention is not limited to such an application an can be used with other connector and cable types such as infiniband , qsfp , hdmi , cfp , cxp and other applications . fig7 d - 7g are perspective views illustrating a method of terminating a double shielded twinax pair according to the present invention , particularly showing : unwrapping the outer shield 104 b ( fig7 d , outer ferrule 122 has already been slid over the outer shield 104 b and back onto the twinax pair out of view ); connecting the twinax pair to a pcb 120 using an inner ferrule 124 ( fig7 e ); rewrapping the outer shield 104 b over the inner ferrule 124 ( fig7 f ); and sliding the outer ferrule 122 over the outer shield 104 b and inner ferrule 124 where it can be crimped or otherwise bonded to the shield 104 b and / or ferrule 124 . outer ferrule 122 can be crimped to electrically bond inner ferrule 124 to the conductive portions of shields 104 a , 104 b . alternatively , inner ferrule 124 can be electrically bonded to the conductive portions of shields 104 a , 104 b by soldering , welding ( ultrasonic or otherwise ), using a conductive adhesive , or by other techniques , which may eliminate the need for outer ferrule 122 . the pair manager and twinax cable according to the present invention provides a low impedance signal return path . inner ferrule 124 is typically connected to a ground pad , or in other words a signal return , on pcb 120 . one advantage of the pair manager according to the present invention is that it can provide broadband improvement in differential return loss for the cable assembly due to more contact with the shield tapes 104 a , 104 b , in addition to providing termination to pcb 120 signal ground or reference , for the shield tapes 104 a , 104 b which tapes provide improved insertion loss characteristics for the cable / assembly according to the present invention . in fig7 h , a cross - sectional side view is shown for a single twinax cable wire - pair . in fig7 i , two options are shown for connecting two wire - pairs 102 to the connector . a cross - sectional view of a standard twinax cable wire par 102 is again shown in fig8 a , and some proposed methods to minimize the shield resonance by moving the drain wire 110 to the side as shown in fig8 b , or through the use of stranded wire as the drain wire 110 located to the side as shown in fig8 c or through the use of two stranded wires located to both sides as shown in fig8 d . locating the drain wire 110 to the side increases the force on the wire and shield to improve the conductivity between them . using stranded wire should improve the conductivity between the drain wire 110 and the shield 104 because the wire can deform to the shape that surrounds it making a better ( lower resistance ) contact . fig9 a and 9b show a way of ensuring a better method of contacting the shield to the drain wire . here a cross sectional view of a twinax cable wire - pair 102 is again shown in fig9 a and a proposed method to minimize the shield resonance by spirally wrapping the drain wire 110 around the wire - pair fig9 b . spiral wrapping the drain wire 110 improves the contact force that the shield tape 104 makes on the drain wire 110 and hence lowers the contact resistance . fig1 a is a cross - sectional view of a twinax cable wire pair 102 and the electro - magnetic field distribution is shown in fig1 b and 10c . due to the boundary conditions at the dielectric air interface , the electric field is distorted ( see b ). this distortion that occurs with the electric field and not with the magnetic field causes an increase of loss to occur within the cable . this is best understood by use of the diagram in fig1 c . the guided energy within the electro - magnetic field is traveling longitudinally along the twinax cable as defined by maxwell &# 39 ; s equation . here the em field must be transverse so as to obtain a minimum loss wave guide . if the electric field distorts , some of the energy is lost due to the fields not being entirely transverse ( this energy is converted to different propagating modes ). fig1 a - 11d illustrate cross - sectional views of various twinax cable wire - pair constructions . in fig1 a , a typical twinax cable wire - pair 102 where each wire is independently formed and is held together in close proximity by the shield tape 104 that surrounds it is shown . the problems with the embodiment of fig1 a include return loss ( where the wires may move apart during cable flexures ), and attenuation ( where some of the energy within the electro - magnetic field is lost at the dielectric air boundary ). both the return loss and the attenuation can be improved through the use of an additional drain wire 110 as shown in fig1 b or either bonding the two wires together as shown in fig1 c or co - extruding the wires together as shown in fig1 d . in the embodiments of fig1 b - d , the amount of energy lost due to electric field discontinuities is minimized . in the embodiments of fig1 c and 11d , the return loss should be improved as long as the manufacturing process keeps the wire - pair &# 39 ; s distance constant . another technique is to begin with circular shaped wires with dielectric and squeeze two wires together which deforms the dielectric into more of a “ d ” shape . another technique of differential signal transmission with improved insertion loss is to utilize two 50ω coax cables . two signals ( who have the same magnitude but 180 ° phase difference between them ) are launched simultaneously into two different coax cables . in this technique , there is a reduction of insertion loss but maintaining a low skew between the two signals can be difficult due to variation in the two different coax cables . for a sfp + application , for example , the present invention can be used in a communication system that includes equipment such as switches , servers , and / or an active patch panel as is described in u . s . patent application ser . no . 12 / 726 , 412 ( nordin et al . ), filed mar . 18 , 2010 , titled “ active patch panel ,” incorporated by reference as if fully set forth herein . the twinax cable can be used in a cable assembly according to the aforementioned patel et al . &# 39 ; 778 patent application , for example , to interconnect various equipment . the present invention can also be used in communication systems of other applications , such as infiniband , qsfp , hdmi , cfp , cxp and other applications employing twinax cable . while particular embodiments and applications of the present invention have been illustrated and described , it is to be understood that the invention is not limited to the precise construction and compositions disclosed herein and that various modifications , changes , and variations may be apparent from the foregoing without departing from the spirit and scope of the invention as described .