/ _8 p" V# T M$ K4 }8 t8 e1 B+ i4 `Cross-talk between FM Broadcast Radio Transmitters (88-108 MHz)' j& r& t# p) I: b& T2 M7 ]2 l* Q
and NMR Spectroscopy: A recent experience& n& y* o. p0 U2 F$ [1 p3 X
6 z3 }& j1 k2 r$ m. L. u- u' r5 e: ?
Recently I had to install a 400 MHz (9.4 T) NMR Spectrometer. The0 j1 Y! H5 J( _# R; U
system worked fine and, using an Indirect Detection Probe , met quickly* r, ]- z- p: G6 D$ G* y% `
and effortlessly the specifications. But later on, when the customer5 z" n/ J+ c* |! @
installed a 13C direct detection Probe, the S/N ratio turned out to be
4 M1 ?* C ^6 z( U( ?) Kquite low and, on top of it, the sensitivity was subject to erratic and H$ L7 c# Y( I$ Q9 I. |
very large variations from 50:1 to 130:1 (manufacturer's specs give5 q1 \/ ]( P# _: W1 [1 Y0 y7 z$ ~- T$ B/ o
155:1), without any apparent reason.
/ m, I: h# Z* {% ~ A Since the nominal 13C observe frequency at 9.4 T is 100,568
4 L4 g$ g! _( m4 sMHz, right in the middle of the range of commercial FM broadcasts, I
- N. M$ Y, U0 |% jhave immediately suspected that the spectrometer was picking up one of1 m$ ^8 P. U* i2 y$ s0 S1 @/ R
those radio stations. In fact, using a cheap FM radio receiver, a
( m$ J5 X0 ~( }! {+ C7 w0 _6 ^; Gstrong station was quickly found at 100,60 MHz. At this point, I have
$ } y: w7 @8 N1 {: T3 rconnected a simple audio amplifier ending with a loudspeaker to the, ^; A/ t% {, ^2 A- Q, ~9 h
output BNC of the observe receiver which was there apparently just for8 s% d) [( E; M
this purpose, and all of us were listening to the radio using a 200.000
. F' [' S! v( E# d5 f7 ~Euro NMR spectrometer, except that the audio quality was really poor,' H2 Z# e2 ]2 P' q1 {: [' v
much worse than from the above-mentioned gadget radio (a shopping mall
) W5 z2 V% f3 ^, R. B% _gift).
- H) L( a X, p The problem is well known from the old times, when the highest
) A) d" P* {$ m9 \1 Gfield was 2.45 T and the nominal H1 frequency was close to 100 MHz. One
& z- d n: R6 q& i4 x6 @5 tof the first Italian NMR spectroscopists to experience it, back in4 T6 `8 M3 {) ~8 D% n6 {
1974, was Prof. L.Lunazzi at University of Bologna, on his brand new
5 m/ F4 ?1 _2 lVarian XL100 spectrometer, and the radio station was Radio San Luchino,
6 v% U3 g5 l: U/ N" L% T1 y) pwell known to anybody living in Bologna, which broadcasts from the top
a1 V# x5 K( j x' S* t( mof the nearby Saint Luca hill.- [3 K! G2 s( t1 e$ x
The obvious solution is to change the magnetic field, and thus
5 K; ^3 l0 p4 C$ f; u$ Sall resonance frequencies, in order to get out of the modulation
( v) m6 E$ C. K* N2 U4 \envelope of the interfering transmitter. But this is not always easy,
! w; i+ j/ a' M; T' D( ysince the range by which one can move the magnetic field changing just9 y, c$ Z7 ]6 i9 H, B2 e" t9 A
some software parameters is usually limited to a few tens of kHz in the, S+ H! `) v% q. K4 j- P2 N
frequency domain. If larger variations are required the poor engineer
" F, l$ u* C Y% K7 y; ]has to work on the superconducting coils of the magnet, which is a
0 F/ \- E7 h2 r2 N9 @9 @; Kno-trivial job entailing the risk of a total or partial quench.
2 t& q2 N" [' n- d% B: N8 N Bitter experience shows that persuading the involved radio
& Z- b* d Z) G6 Z7 nstation to change its operating frequency is a time consuming,
" x4 w( c6 M G! Q3 ]frustrating, and apparently quite impossible task.* ?( G8 ~8 u, P0 `$ _
Being well aware of the problem, my preliminary spectrometer! c! h& ]. H; x6 D
checks always include some blank acquisitions taken before running up
* u5 V4 o5 F$ l2 Z* P+ J& d$ I# Dthe magnet so that there is no chance to observe an NMR signal. The
4 d Z( z( e* v) f: cresulting dataset should be pure white noise, without significant
" B4 p% F# C% n) S) yspikes. This was done also in this particular installation but, as- ?1 L! V/ T% ^4 I, Z M2 H
usual, in the days following the energization the magnet drifted a bit,
2 l0 c) `9 Q* }* V3 a' g H) D6 X/ |getting closer to the radio station carrier. Furthermore, the usual 13C
* W1 V- Y# X+ p3 s" z jspectral widths are quite wide which makes things even worse. Murphy's
2 F6 g" j' v# A9 iLaw has no exceptions!
/ _" _( C3 g" _ But we are just at the beginning of my real troubles. Before
) K5 d) ?+ _& ]! M: K+ N, p+ Lputting one's hands on the magnet, one should better know how much, in1 A2 ~* b$ [% x5 l
which direction, should the field be moved. I have therefore used a/ ~# S1 A$ D, ]8 v# |& o; }
good Spectrum Analyzer (Tektronix model 2710) to check the frequency
7 g% [# y6 Y7 Z8 q% T% sspectrum around 100 MHz, ready for the worst. And the worst was what I
$ n; l- z9 I) X7 E6 S/ Wgot! The band was filled with FM signals, evenly spaced by 250 kHz and7 u. x. c' i; D5 G$ I, O
with modulation envelopes as wide as 100 kHz, so that when I got far. ~. L9 I) @2 X3 i
from one station I started receiving the next one; accounting for
; _4 C3 B3 {9 q' M8 X Rfolding and aliasing effects, there was no chance! The only somewhat
# V- Z; M) B3 {7 M) O- h. ]7 Qfree region was at 100,120 MHz, but this implied proton frequency of
9 v1 m2 [+ `3 J398.100 MHz. So now the spectrometer is no longer a "400"!# \1 e8 y6 ]' `
Before installing a spectrometer, you better get a Spectrum9 B0 _# b* E; \, T5 K; a, K
Analyzer and check for the presence of RF fields in the instrument
) O& `- L+ l2 U- [1 m! \room, taking care to explore the areas close to the observe frequencies- f. g8 G' \* X- I, C$ X) V
of all the most important nuclei. Don't forget the lock: at 14 T" E9 }2 a! X7 P8 o- P" j/ W
(nominal 1H frequency of 600 MHz) 2H resonates at 92,095 MHz, once, @, g5 d8 y/ s0 y! R/ P* R
again in the FM broadcast band. The lock channel receiver has quite
5 h, e4 `& P) u# wnarrow bandpass filters, so hitting a radio is a really bad luck, but
: o( H5 x/ O' `2 v2 zit had already happened, resulting in fast lock level variations and
. `# u$ w. ~( h" @totally malfunctioning Gradient Shimming which uses deuterium as
) z" X2 g2 i7 g' J8 e- C1 |$ oobserve nucleus!
$ F% M1 ~6 }& `3 w" g/ ] Needles to say, the extremely high sensitivity of an NMR8 _: a& w5 ~' i4 E' W
Spectrometer shows up. The signal from the guilty radio, as observed on* S# _* {# k6 h% q9 j% d* X
the spectrum analyzer inside the spectrometer room, had very low1 }5 M. G! e; V$ s- g
intensity level of about -70 dBm, some microvolt/meter, but that was! ?( A( z7 c& I% f, r0 m6 Q
enough to almost completely hide the quite strong 13C signal from the
2 F M4 a& ?0 T. g6 PASTM sample!
9 `4 b" R2 P. a' T( W: ` The radio was clearly picked up by the Probe (closing the
* u+ @. Q* r* N$ x, R5 F2 xPreamplifier input with a shielded 50 ohm RF load, all signals
) d) I |$ ]7 o2 \2 T4 E+ T Ydisappear) but, quite surprisingly, there is almost no shielding effect
8 A8 `* M" l2 ~+ sattributable to the metal body of the magnet, which is after all an
( Q* \2 @# x, A6 q1 G* G! ?almost completely closed cylinder all around the Probe. Most probably a, P% ] Q) ]* C! [! Y5 h
good deal of the signal leaks in through the Shim Coils which are+ z3 x2 I y& {7 u. U/ D
mounted very close to the Probe and, together with their connection
3 @+ K% u, K, P& f8 vcables to the Console, constitute a quite good antenna.
% {. t, `+ i1 K Too bad the Shim Coils are essential, and effective shielding
" m- s' c3 P6 U1 uof the instrument with a Faraday's cage is always difficult and
2 u% W- i# Z" s, J F# Sexpensive (it may be almost impossible once the spectrometer is8 I0 a; M. b5 E
installed).
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Before concluding, let me venture some additional advice based on my experience:/ Y* K9 f" e0 G
1 R; `9 b9 P2 q( n9 P
= Install the spectrometer in the best shielded room& W( y* `0 {% Z. v" b) U
you can get; the best choice is once again in the basement, where you
( ^0 }, l) i' N6 g9 X+ Dhave the whole building above the ceiling and its [grounded]
/ `2 N% [3 ~; [" s5 j4 G3 ^foundations all around the rest, done in iron-reinforced concrete,
: M g6 Q p2 _* X% J+ A1 l, ^amounting to a good Faraday's cage at no extra cost.* _# r' Z& B8 _1 _2 `5 n/ {
+ {' K( b J) a1 f# W
= If possible, avoid top floors. If you can't avoid+ j$ ?0 m' ~9 I' L
going upstairs, take a good look out of the window: if you see nearby
& g' Q9 ]! b% ltransmission antennas, get ready for troubles proportional to their1 O- V" r0 u0 Y4 E
dimensions and closeness (to my knowledge, however, mobile telephony
, N- l- D# q5 vantennas cause so far no harm)., c2 i( Y* k7 |( \+ A
! p& G% L2 b; r9 U* k= I'm sure that an exchange of experiences and/or( T+ Y4 Y6 B* V8 y! A
suggestions regarding this matter would help a lot to solve many" s$ }1 t4 o9 x9 v
existing installation problems and prevent ones yet to come. Stan's Blog is an ideal location and, needless to say, I will be absolutely glad to cooperate.
( p" o) f( r! S: l- n# L2 K2 Z
6 C2 m" u' M/ v1 h% DVanni Piccinotti, Firenze, 11 April 2008
摘自stan' NMR Blog.
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