| // Represents a single cavity mode | |
| // Larry Doolittle, LBNL, May 2014 | |
| // Uses up six multipliers | |
| // Fabric use is dominated by two 18-bit fully unrolled CORDIC processors | |
| // Intended to be clocked at twice the ADC clock rate, should work | |
| // at full speed in any of V5, V6, A7, K7. Should come close on S6. | |
| // This covers the electrical side, and includes an interface to the | |
| // mechanical side (mech_freq, v_squared). | |
| // The expectation is that several of these modules will be instantiated, | |
| // one per passband mode (or at least the top two). Their field and | |
| // reflected outputs will be summed (and note the individual control on | |
| // the phase of these contributions). The final reflected wave will | |
| // also include a direct reflection component from the forward wave. | |
| // Also, coarse (many cycle) delays need to be constructed. The drive | |
| // to this module should include the beam-loading component (which does | |
| // not get reflected). | |
| // At some point, we want to add the ability to simulate a quench. | |
| // Per-mode memory map: | |
| // 0 not used | |
| // 1 m_coarse_freq (see cav_elec.v) | |
| // 2 drive_coupling | |
| // 3 bw | |
| // 4-7 out_couple | |
| // Synthesis places this in the 4.8 ns range (on a '7A100T-2), | |
| // pretty far from what I think should be the 3.8 ns limit from the | |
| // CORDIC elements. The IIR element in lp_pair tests by itself at | |
| // 3.0 ns, so that's not it. | |
| module cav_mode( | |
| input clk, | |
| // Input signal on waveguide given in IQ form | |
| input iq, // high for I, low for Q | |
| input signed [17:0] drive, // High power amplifier only | |
| input [11:0] beam_timing, // common to all modes | |
| input [18:0] lo_phase, // should change every other cycle, see below | |
| // Field probe and reflected wave signals at 20 MHz IF, interleaved | |
| output signed [18:0] probe_refl, | |
| input [18:0] beam_phs, | |
| // Coupling to mechanical system | |
| // mech_freq step size is 94.3 MHz / 2^32 = 0.022 Hz, | |
| // range is +/- 2^27 steps = +/- 2.9 MHz from nominal 1300 MHz | |
| // (adequate to represent 8pi/9 and 7pi/9 modes). | |
| input signed [27:0] mech_freq, | |
| output signed [17:0] v_squared, | |
| (* external *) | |
| input signed [17:0] drive_coupling, // external | |
| (* external *) | |
| input signed [17:0] beam_coupling, // external | |
| (* external *) | |
| input signed [17:0] bw, // external | |
| `AUTOMATIC_self | |
| ); | |
| `AUTOMATIC_decode | |
| parameter shift=18; // passed transparently to lp_pair.v | |
| // Compute beam drive magnitude | |
| // Wastes at least half a multiplier | |
| reg signed [29:0] beam_mag_wide=0; | |
| always @(posedge clk) beam_mag_wide <= beam_coupling * $signed({1'b0,beam_timing}); | |
| wire signed [17:0] beam_mag = beam_mag_wide[21:4]; // XXX cheat scaling? | |
| // Phase accumulator from mechanical system | |
| reg signed [31:0] mech_phase_fine=0; | |
| always @(posedge clk) if (~iq) mech_phase_fine <= mech_phase_fine + mech_freq; | |
| wire [18:0] mech_phase = mech_phase_fine[31:13]; | |
| // Half the CORDIC cycles will be used to compute the drive coupling, | |
| // and the other half will compute the beam loading vector. | |
| reg signed [17:0] cordic_x = 0; | |
| always @(posedge clk) cordic_x <= iq ? beam_mag : drive_coupling; | |
| reg [18:0] cordic_phs = 0; | |
| always @(posedge clk) cordic_phs <= mech_phase + (iq ? beam_phs : 0); | |
| wire signed [17:0] xout, yout; | |
| cordicg_b22 #(.nstg(20), .width(18)) icordic(.clk(clk), .opin(2'b0), | |
| .xin(cordic_x), .yin(18'b0), .phasein(cordic_phs), | |
| .xout(xout), .yout(yout)); | |
| // Buffer layer, generates Re/Im sequential pair from CORDIC output. | |
| // Note that a consistent pair should come from a single value of lo_phase. | |
| reg signed [17:0] yout_d=0, mul_coef=0, beam_drv=0; | |
| always @(posedge clk) begin | |
| yout_d <= yout; | |
| mul_coef <= ~iq ? xout : yout_d; | |
| beam_drv <= iq ? xout : yout_d; | |
| end | |
| // Vector multiply drive by the time-varying vector to convert it | |
| // from reference coordinates to cavity-centered coordinates. | |
| wire signed [17:0] mul_result; | |
| complex_mul in_couple(.clk(clk), .gate_in(1'b1), .iq(iq), | |
| .x(drive), .y(mul_coef), .z(mul_result)); | |
| // Depend on the fact that when the beam loading input magnitude is zero, | |
| // the CORDIC output is precisely zero, and therefore doesn't contribute | |
| // to roundoff error. | |
| // One cycle delay aligns real and imaginary parts with amplifier drive. | |
| reg signed [23:0] drive2=0; | |
| always @(posedge clk) drive2 <= {beam_drv,6'b0}; | |
| // Now that we're in the natural coordinates of the cavity resonance, | |
| // the cavity itself is just a vector IIR low-pass filter. | |
| wire signed [17:0] res; | |
| lp_pair #(.shift(shift)) lp_pair(.clk(clk), .drive(mul_result), | |
| .drive2(drive2), .bw(bw), .res(res)); | |
| // Two channels of output coupling, field probe and reflected wave. | |
| // Also upconverts to IF, as provided by lo_phase input. | |
| reg [18:0] out_phase=0; | |
| always @(posedge clk) out_phase <= lo_phase - mech_phase; | |
| (* lb_automatic *) | |
| pair_couple out_couple // auto | |
| (.clk(clk), .iq(iq), | |
| .drive(res), .lo_phase(out_phase), | |
| .pair(probe_refl), | |
| `AUTOMATIC_out_couple | |
| ); | |
| // square and (1+z^{-1}) filter res, goes to v_squared | |
| wire signed [18:0] mag2; | |
| mag_square square(.clk(clk), .iq(iq), .d_in(res), .mag2_out(mag2)); | |
| // mag2 is guaranteed positive! | |
| assign v_squared = mag2[18:1]; | |
| endmodule | |