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DCHPPA Stage 2: IF Signal Processing Circuit Configuration

5. DHCPPA Experimental Implementation and Practical Results

5.4 DCHPPA Circuit Configuration and Practical Result

5.4.1 DCHPPA Stage 2: IF Signal Processing Circuit Configuration

The idea of the DCHPPA design, based on the super heterodyne principle, exists in

conventional RF/MW radio receiver, which is still the most popular technique since it was

invented in 1918. In the superheterodyne, dual, down-conversion mixing technique is used

as shown in figure 5.14.

Figure 5.14 System diagram for super heterodyne double down conversion

Also the heterodyne approach has been seen as a very attractive technique for an

optical SCM system, particularly in terms of a long haul application; it can also be more

applicable for a free space application, as seen in this chapter. In the SCM optical receiver,

as shown in figure 5.15 [75], the optical signal can be detected by the PD and then

amplified by a low noise amplifier LNA, which results in amplification of all the received

signal (i.e desired and non-desired signals), including the PD noise occurring due to the

optoelectronic signal converter. These output signals will feed to the mixer for down or up-

PORT1 P=1 Z=50 Ohm Pwr=-50 dBm PORTFN PORTF

FET LNA

Mixer-1

1st IF Filter

IF Amp

Mixer-2

LBF

Amp

LO-1

LO-2

PORT P=4 Z=50 Ohm BP SUBCKT SUBCKT NL_AMP2 NL_AMP2 DLPFC RF IN IF OUT LO MIXER RF IN IF OUT LO MIXER 10

will feed again into the second up/down mixer, which aims to recover the original

baseband signals to achieve better gain and better receiver sensitivity. In general, the

multiple conversion technique has been shown to work well in many RF/MW receivers,

but it is more complicated compared to a simple photo-detection circuit.

Figure 5.15 System diagram for a microwave-multiplexing light wave system

The DCHPPA acts in a parallel manner to a conventional double superheterodyne

detector system, but without the noise penalty that normally occurs. Photoparametric

amplification is used at the first stage instead of a resistive/transistor-based mixer or

preamplifier front end circuit. In this section, the practical demonstration of the DCHPPA

will be presented. Figure 5.16 shows the circuit configuration of the DCHPPA receiver.

Each stage requires careful consideration of the choice of components. The whole circuit

was divided into three stages, each stage with its sub-circuits; the PPA circuit stage 1,

which includes passive LC band pass filter circuit and the photo detector circuit as

explained in previous section; IF Signal processing stage two, which includes the pre

selector cascading band pass filters followed by an IF amplifier circuit, followed by a

PINDD SDIODE

NL_AMP2

Microwave power combiner Subcarrier modulator

LO

Microwave receiver Single-Mode Fiber Baseband -1 fsc1 fsc N Analog or digital video

LASER PHOTODIODE FET LNARF IN IF OUT LO

MIXER

PORTFN PORT

second IF cascading bandpass filters; down converter mixer stage 3, which includes a

passive LC bandpass filter circuit and DBM circuit, followed by a low pass filter.

As illustrated in the graph, the same pump source (LO) was used for the up-

converter and down-converter via a 2-way, 0 degree power splitter (i.e. no phase shift)

device. The LO was injected via high quality band pass filters that provide a convenient

method of applying the pump to the PD ( i.e. mixer one) as well as the DBM circuit (i.e.

mixer two), whilst at the same time providing isolation, reducing LO sideband noise and

blocking dc components from passing through. The up-converter mixer works to convert

an RF signal (1MHz) to the first upper sideband signal IF (RF+LO; 433.92MHz), where

432.92MHz was used as the LO pump frequency. The down-converter mixer works to Figure 5.16 Experimental arrangement of the DCHPPA

Stage-1 Stage-2

recover the desired baseband channel (1MHz) from the IF signal (433.92MHz). A picture

of the final setup can be seen below in figure 5.17.

As mentioned before, the signal processing stage two required a considerable

amount of attention; in particular with respect to selectivity and sensitivity, the most

important in this stage is selectivity; however, sensitivity is also desirable. In contrast,

there are four frequencies in the PPA output spectrum (ωp,ωs,ωp±ωs) with their

harmonics (i.e third and fifth order; ωIF=mωs±nωLO) at various level of powers. As shown in figure 5.5(b). At 22dBm pump power, the LO signal level (i.e. 432.92MHz) was

measured over the PD to about 10dBm using a spectrum analyzer.

Figure 5.17 Final DCHHPA system set-up

At high pump, the LO signal over the PD can lead to serious drawbacks if its PD output is

connected to the following stages without drastic consideration. For example, it can

saturate the DB mixer (mixer two) due to a high level of input power, as well as forcing the

SAW BPF to an unstable condition or damage. Therefore minimizing the LO level of

power at the PPA output is one of the key considerations; a limiter circuit was used to

reduce this effect; however, due to both frequencies (i.e. 432.92MHz and 433.92MHZ)

being close to each other (e.g. almost commensurate frequencies), the desired IF harmonic

was affected as it is weaker than the LO.

In addition, the preselector IF SAW filter should have two primary functions, one

being to accept a high input power, such as LC passive filters and ceramic filters.

Secondly, it must provide high selectivity with low insertion loss, such as a Crystal filter

[142]. A high-Q commercial Crystal filter was used in a previous published paper [143] at

the VHF frequency range. The filter was from Filtronics INC (FN-3809) with a 240MHz

centre frequency and 100 KHz pass bandwidth. The input power level was up to 5dBm,

and it exhibited a good frequency response as shown in figure 5.18a. Although it showed

high selectivity, it can be unstable at high pump power and economically, it is very

expensive (i.e. 250$) (see Appendix B7 for schematic circuit). Most of the present-day

crystal filters start being unstable when the input power exceeds zero dBm, and may result

in poor performance, as reported in [81] .

Ambitiously, a Surface Acoustic Wave (SAW) filter may overcome the previous

issues with respect to selectivity, rejection, low loss, input power and cost (i.e. less than

2$), employing such components offering substantial yet affordable benefits in the access

network. Also it was shown to work well in both analogue and digital transceivers (i.e.

AMPS, GSM) with a very good performance for frequency/phase noise, and it exhibited

long term stability [144, 145]. Several SAW filters were implemented and tested for better

selectivity performance. Two narrow band commercial SAW BPF filters with 120KHz

between the filters to compensate for the capacitive part of the filter impedance (see

Appendix B8). The designed ultra narrow band pre IF filter aims to provide greater

steepness to the filter edge and high selectivity, while maintaining low insertion loss, as

shown in figure 5.18b. Moreover, it provides high stability, cost effectiveness and a better

frequency response performance compared to the Crystal Filter, as illustrated in figure

5.18a.

The pre IF SAW filters were used and performed as a good preselected to pass only

the desired IF signals, remove the noise outside its bandwidth, and also eliminate other

odd- and even mixing products from breaking through. Moreover, these provided high

isolation for unwanted frequencies, such as RF and LO, which could cause additional

distortion products, and which are reduced in severity. High selectivity and low insertion

loss are more desirable at this stage.

The IF amplifier in stage two is responsible for providing additional gain to the

receiver to render incon sequential any noise introduced in the subsequent stages, as well

as providing isolation by rejecting the reflect power form subsequent stage to pass back to

the pre IF SAW filter. A mini-circuit variable LNA (ZFL-500LN) was used with 24db gain

and 2.9dB noise figure. This amplifier can be used as what is known as an Automatic Gain

Controller amplifier (AGC) at IF stages, which consists of a variable-gain amplifier and

automatic gain controller mechanism that keeps the output swinging constantly over a wide

range of input swings, and which seems to be more desirable for diffuse and quasi-diffuse

optical links, particularly for mobile wireless receivers where the incident detected power

signal may vary, due to mobility. In general, any appreciable amplitude with very low

noise figure is desirable at this stage; two mount surface mini-circuit IF amplifiers (TAMP-

and successfully implemented and tested; each amplifier has almost about a 20dB gain; the

cascaded IF amplifiers resulted in 40 dB gain overall (see appendix B9).

a) crystal filter (4.9dB insertion loss);

In the third step in stage two, the LO signal is still the main cause of the distortion

products, even if it has been minimized in the previous stage; therefore a cascading of two

ultra narrowband SAW filters (Epcos-B3790, +5dBm input power) in series were designed

and connected in series and matched to 50Ω impedance to be used as a post IF filter (see

Appendix B10). The high ultra narrowband post IF filter aims to provide greater steepness

at the filter edge and high selectivity, as shown in figure 5.18c; and pass only the desired

IF signal whilst suppressing all other LO, harmonics and noise signals, as seen in the next

practical results section.