In all the studies involving microinjection of fluorescent RNA into
the nucleus, the RNA was very soon thereafter observed at its sites
of intracellular concentration, e.g. the nucleolus for RNase MRP
RNA, RNase P RNA, SRP RNA and various other small nucleolar RNAs
(
7,
8,
11,
12,
19–
25)
or at interchromatin granule clusters for pre-mRNA (
4,
27). However, it was not feasible in any
of these numerous studies to capture the actual movement of the
RNAs, in part because it was so fast.
In an important advance, Politz
et al. (
31) showed that oligo(dT) introduced into
rat myoblasts becomes hybridized to poly(A) RNA, based on an
in
situ oligo(dT)-primed reverse transcription assay (
31,
32).
This was the first compelling demonstration that an oligonucleotide
introduced into living cells actually hybridizes to complementary
RNA sequences. Subsequently, fluorescence correlation spectroscopy
(FCS) revealed that the fluorescent oligo(dT) inside the nuclei
of living rat myoblasts moved at rates expected if the probe were hybridized
to poly(A) RNA molecules that were moving by diffusion (
33). Moreover, the movement was unaffected
when ATP levels were pharmacologically reduced (
33).
Fluorescence recovery after photobleaching (FRAP), an established
method for measuring the diffusion of molecules in living cells,
gave results very similar to those determined by FCS microscopy (
33). These findings bolstered confidence
in the RNA-hybridized state of the fluorescent oligo(dT). However,
although these FCS and FRAP studies provided a rigorous interrogation
at the microscopic physical scale of molecular dynamics, the goal
of actually watching RNA movement in living cells, in real time, remained
a challenge.
The next step in the fluorescent RNA cytochemistry field involved ‘caged’ fluoresceins,
a family of compounds initially synthesized by Timothy Mitchison
(
34). In these caged fluoresceins,
two
O-nitrobenzene groups attached via ether linkages lock
the fluorescein into its non-fluorescent tautomer (
35). These
caging groups can be split off by 360 nm photolytic cleavage, resulting
in native fluorescein (λ
ex = 418
nm).
Politz
et al. (
36)
found that oligo(dT) labeled with this caged fluorescein had cellular
uptake and poly(A) RNA hybridization properties similar to (non-caged)
fluorescent oligo(dT). The intranuclear movement of poly(A) RNA
was then investigated, using caged fluorescent oligo(dT) followed
by localized uncaging in a defined intranuclear volume by 360 nm
light brought in through a 1.5 µm aperture
in the microscope condenser from an argon multiline laser, so that
the uncaged probe bound to poly(A) RNA could be tracked as a bright signal
moving out into (initially) dark surrounding regions of the nucleus
(
36). These experiments were
made possible by a very rapid image acquisition fluorescence microscopy
technology (
37,
38).
It was found that the poly(A) RNA signal moved out from the uncaging
site in all directions and eventually occupied all of the nucleus
except for the nucleoli, from which it was excluded. When the DNA
in these cells was stained with Hoechst 33342 and imaged relative
to the distributed poly(A) RNA, it was found that the majority of
the RNA was located between the interphase chromosomes. These results
demonstrated that poly(A) RNA moves randomly in the nucleus. Additional
data indicated that this movement is independent of temperature
between 23 and 37°C, which is compatible
with a diffusion-based process in which metabolic energy is not
limiting (
36), and supports the FCS
and FRAP results (
33).
The nuclear poly(A) RNA tracked in these experiments contains
multiple biosynthetic classes, including pre-mRNA as well as some
nucleus-restricted poly(A) RNAs of unknown function. Therefore it
was not certain whether the observed random, diffusion-like movement
reflected the productive pre-mRNA→mRNA
pathway, the behavior of nucleus-restricted poly(A) RNAs, or both.
However, a subsequent study of the intranuclear movement of a specific,
well-characterized pre-mRNA, which undergoes splicing and is exported
to the cytoplasm as a
bona fide messenger RNA,
revealed that this transcript moves away from the gene in a random
walk fashion characteristic of diffusion (
39,
40). Additional evidence for export of
a specific mRNA over the entire array of nuclear pores has been
reported (
41,
42).
The picture that emerges is one of processed mRNAs moving out into
the interchromatin space by diffusion, then encountering specific
binding proteins that create an ‘export me’ ribonucleoprotein
signature (
42), with the resulting
RNP complexes then stochastically encountering the (highly complex)
nucleoplasmic side of the nuclear pore machinery (
43).
It is to be noted that several recent studies on the movement of
proteins within the nucleus have also revealed a pattern of rapid,
random, ATP-independent motion indicative of diffusion (
44,
45),
suggesting that whatever organized structure exists in the interchromatin
space (
44,
46,
47) it does not appear to contravene the
movement of RNA or proteins as a process that appears to be mechanistically one
of diffusion, however constrained by the plausibly crowded intranuclear
environment.
A third approach recently introduced to track the movement and
localization of RNA in living cells involves the expression of a
green fluorescent protein (GFP)-tagged protein that binds to a specific
RNA target sequence (
48). The
chief appeal of this method is that it lends itself to the now quite
routine practice of expressing GFP fusion proteins in a wide variety
of cells. This method was initially applied to track a specific
mRNA in living yeast cells (
48)
and has more recently been applied to follow mRNA transport in cultured
rat hippocampal neurons (
49). Each
of these approaches has inherent advantages and limitations. Microinjection
of fluorescent RNA requires a certain degree of manual adroitness,
although this skill is readily acquired by most who undertake it.
The use of caged fluorescent oligonucleotides to track RNA depends
on good cellular uptake and productive hybridization, and requires
ultra-fast image acquisition microscopy expertise (
37,
38). The method, based on GFP protein
binding to RNA targets, requires that the GFP protein expression
level operates in a RNA titration mode (i.e
. the
method is compromised if there is an excess of the GFP protein not
bound to RNA), although this has been addressed in a subsequent
version of the method that has been developed (
50).
Moreover, in each of these methods the fact that the reporting RNA
is derivatized must be borne in mind. With microinjected RNAs there
is a fluorochrome every 40 nt or so. With caged fluorescent oligonucleotides
the targetted RNA has short double-stranded regions of hybridized
oligo beyond the RNA’s inherent secondary structure and
it is possible that this exerts some influence on the observed movement.
In the GFP protein-based method, the RNA target contains six or
more inserts of a bacteriophage RNA sequence and thus potentially
has multiple RNA binding proteins attached, thus itself constituting
a ribonucleoprotein particle, although for some purposes the number
of protein binding sites can be reduced (
50,
51). Thus, these three methods involve increasing
chemical derivatization and attendant molecular mass in the order
they are mentioned above, and yet have decreasing experimental complexity
in the same stated sequence.