### Table 2: Wakefields due to the vacuum chamber rough- ness in several Linear Collider components. Parameters are listed in 4.

### Table 1 Main parameters of the S-band 500 GeV (c.m.) linear collider.

### Table 1: Estimation of minijets for 0.5 TeV Linear Colliders at LC92 together with the collider apos;s parameters, where the luminosities are given along with the enhancement factors.

### Table-1. Machine Parameter of C-band Linear Collider ------------- Basic Parameters ---------------------------------------- Center of Mass Energy GeV 500 1000

### Table 1: New parameters of the TESLA 500 GeV (c.m.) linear collider in comparison with the original design.

### Table 1. Characteristics of small amplitude internal waves from linear theory, and

"... In PAGE 4: ... #283#29 results in an eigenvalue problem which can be solved to give the dispersion relation for small-amplitude internal waves #28for example, see Gill #281982#29#29: ! 2 = N 2 k x 2 j ~ kj 2 = N 2 cos 2 #02: #284#29 The group velocity of the waves can be determined from this expression and therebyit can be shown that #02 represents the angle of propagation of the waves to the vertical. The polarization relations and other relevant properties of internal waves are listed in Table1 . For consistency with the results presented here, amplitudes of various #0Celds are given in terms of the amplitude A w of the vertical velocity #0Celd.... In PAGE 7: ... Although the incidentwavepacket may be stable to self-acceleration e#0Bects, the superimposed in- cident and re#0Dected waves are unstable if the amplitude of the incidentwave exceeds A w crit =2. That is, if A w #3EA w break = #10 2 ,1=2 sin #02 cos 2 #02 #11 N k x : #2811#29 Table1 summarises the #0Cnite-amplitude stability regimes described in sections 2. #28b#29 and #28c#29.... In PAGE 11: ... The wavepacket is of rela- tively small amplitude, A w =0:02N=k x . The #0Celd is normalised by the maximum initial value of huwi #28see Table1 #29. A horizontal dashed line is drawn to indicate the heightof the re#0Dection level #28the height where the Doppler-shifted frequency of the wave equals the buoyancy frequency N#29.... In PAGE 11: ... Figure 3b illustrates the structure of the re#0Dected waves at time t apos; 48T. The plot shows contours of the vertical displacement #0Celd, #18, normalised by the maximum value of this #0Celd at time t = 0 #28see Table1 #29. The hori-... In PAGE 22: ...s in Fig. 2, Fig. 11 shows time series of ,h#10#18i, computed for simulations of small- and large-amplitude horizontally compact wavepackets with a,d#29 k z = ,0:4k x , b,e#29 k z = ,0:7k x and c,f#29 k z = ,1:4k x . Each time series is normalised by the predicted maximum initial value of ,h#10#18i #28see Table1 #29. In the small-amplitude cases, the horizontally compact and periodic waves show sim- ilar behaviour.... ..."

### Table 4: Current values of some important electroweak parameters, and the potential uncertainty obtainable at a linear collider providing with high statistics (e.g., 109 Z0 decays).

"... In PAGE 47: ... For example, one could improve the current precision on the forward-backward asymmetry parameter Ab by more than an order of magnitude. In Table4 , we have listed some improved measurements envisioned at the linear collider. The tiny error on sin2 e W assumes a precise beam polarization measurement that may require polarizing both the electron and positron beams.... ..."

### Table 1.1: The physics spectrum that can be explored in experiments at e+e? linear colliders with energies extending from LEP up to 2 TeV.

in Contents

### Table 5: Sensitivity of e+e? linear colliders and the LHC to e ects of a Z0, after [125]. The table gives the mass reach in TeV for observability at the 95% CL. The analysis for linear colliders is based on measurement of indirect e ects for an event sample of 200 fb?1; it includes the e ect of experimental cuts. The analysis for the LHC gives the direct sensitivity to a resonance, assuming an event sample of 100 fb?1 and Z0 decays only to Standard Model fermions.

"... In PAGE 53: ... All of the special handles of the e+e? environment, including polarization asymmetries, avor tagging, and polarization, can be brought to bear in the search for these interference e ects. Table5 , based on [125], gives a comparison between the sensitivity of e+e? linear colliders and that of the LHC. The models listed in the table correspond to particular choices for the quantum number assignments of the Z0; see the original reference for details.... In PAGE 55: ... These would appear as Z0 bosons. The sensitivity of the LHC and the linear collider to these states is greater than that to the `SSM apos; (Sequential Standard Model) boson listed in Table5 . If several states can be discovered, one can begin to map out the geometry of the extra dimensions.... ..."

### Table 5: Sensitivity of e+e? linear colliders and the LHC to e ects of a Z0, after [125]. The table gives the mass reach in TeV for observability at the 95% CL. The analysis for linear colliders is based on measurement of indirect e ects for an event sample of 200 fb?1; it includes the e ect of experimental cuts. The analysis for the LHC gives the direct sensitivity to a resonance, assuming an event sample of 100 fb?1 and Z0 decays only to Standard Model fermions.

"... In PAGE 53: ... All of the special handles of the e+e? environment, including polarization asymmetries, avor tagging, and polarization, can be brought to bear in the search for these interference e ects. Table5 , based on [125], gives a comparison between the sensitivity of e+e? linear colliders and that of the LHC. The models listed in the table correspond to particular choices for the quantum number assignments of the Z0; see the original reference for details.... In PAGE 55: ... These would appear as Z0 bosons. The sensitivity of the LHC and the linear collider to these states is greater than that to the `SSM apos; (Sequential Standard Model) boson listed in Table5 . If several states can be discovered, one can begin to map out the geometry of the extra dimensions.... ..."