A howland current source does not require a second buffer op-amp if the desired output current is only 1.5mA, and with careful selection of resistors, the positive +5V supply can be used as the reference voltage. Resistor Rs is your PT100:
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This requires \$R_3 = R_4\$, so that:
$$ I_{OUT} = \frac{5V}{R_3} $$
This has the problem that any noise present on the +5V supply rail will be injected into the signal, and some fraction of it will appear at the output. If you have a precise and clean +5V supply, then that's not a problem, but a noisy supply (like a DC-DC converter output) would require that you produce some precise ground-referenced and low-impedance source. Here I use the TL431 to produce exactly +2.5, and adjust R3 and R4 to suit:
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The above solutions require the op-amp to be powered from both positive and negative supplies, since the OPA2209 op-amp cannot operate with inputs close to the negative supply. See the bottom of page 6 of the the OPA2209 datasheet, a parameter called "Common-mode voltage range". The op-amp inputs in the above design hover at +150mV, very close to ground potential, meaning you can't use ground as the op-amp's negative supply.
If this is the only part of your system using the −5V supply, then you can simplify the design by using an op-amp with a wider acceptable input voltage range, such as the LM358, which will work well with input voltages right down to its own negative supply potential. That can then be 0V (ground), instead of −5V.
Doing that, the op-amp won't be able to output 0V. An LM358 will certainly get its output below +100mV, corresponding to sense resistance \$R_S\approx 30\Omega\$, at a temperature of about −170°C.
If precision isn't so important, consider these transistor-based
designs:
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Adjust R2 to set current:
$$ I_{OUT} \approx \frac{0.7V}{R_2} $$
This is variation in \$I_{OUT}\$ as supply voltage varies from +4.8V to +5.2V:
This is how \$I_{OUT}\$ changes as PT100 resistance \$R_S\$ varies from 50Ω to 500Ω: