Difference between revisions of "Hebb rule"
(Importing text file) |
Ulf Rehmann (talk | contribs) m (tex encoded by computer) |
||
Line 1: | Line 1: | ||
+ | <!-- | ||
+ | h1101001.png | ||
+ | $#A+1 = 45 n = 0 | ||
+ | $#C+1 = 45 : ~/encyclopedia/old_files/data/H110/H.1100100 Hebb rule, | ||
+ | Automatically converted into TeX, above some diagnostics. | ||
+ | Please remove this comment and the {{TEX|auto}} line below, | ||
+ | if TeX found to be correct. | ||
+ | --> | ||
+ | |||
+ | {{TEX|auto}} | ||
+ | {{TEX|done}} | ||
+ | |||
''Hebbian learning'' | ''Hebbian learning'' | ||
− | A learning rule dating back to D.O. Hebb's classic [[#References|[a1]]], which appeared in 1949. The idea behind it is simple. Neurons of vertebrates consist of three parts: a dendritic tree, which collects the input, a soma, which can be considered as a central processing unit, and an axon, which transmits the output. Neurons communicate via action potentials or spikes, pulses of a duration of about one millisecond. If neuron | + | A learning rule dating back to D.O. Hebb's classic [[#References|[a1]]], which appeared in 1949. The idea behind it is simple. Neurons of vertebrates consist of three parts: a dendritic tree, which collects the input, a soma, which can be considered as a central processing unit, and an axon, which transmits the output. Neurons communicate via action potentials or spikes, pulses of a duration of about one millisecond. If neuron $ j $ |
+ | emits a spike, it travels along the axon to a so-called synapse on the dendritic tree of neuron $ i $, | ||
+ | say. This takes $ \tau _ {ij } $ | ||
+ | milliseconds. The synapse has a synaptic strength, to be denoted by $ J _ {ij } $. | ||
+ | Its value, which encodes the information to be stored, is to be governed by the Hebb rule. | ||
− | In [[#References|[a1]]], p. 62, one can find the "neurophysiological postulate" that is the Hebb rule in its original form: When an axon of cell | + | In [[#References|[a1]]], p. 62, one can find the "neurophysiological postulate" that is the Hebb rule in its original form: When an axon of cell $ A $ |
+ | is near enough to excite a cell $ B $ | ||
+ | and repeatedly or persistently takes part in firing it, some growth process or metabolic change takes place in one or both cells such that the efficiency of $ A $, | ||
+ | as one of the cells firing $ B $, | ||
+ | is increased. | ||
Hebb's postulate has been formulated in plain English (but not more than that) and the main question is how to implement it mathematically. The key ideas are that: | Hebb's postulate has been formulated in plain English (but not more than that) and the main question is how to implement it mathematically. The key ideas are that: | ||
Line 9: | Line 29: | ||
i) only the pre- and post-synaptic neuron determine the change of a synapse; | i) only the pre- and post-synaptic neuron determine the change of a synapse; | ||
− | ii) learning means evaluating correlations. If both | + | ii) learning means evaluating correlations. If both $ A $ |
+ | and $ B $ | ||
+ | are active, then the synaptic efficacy should be strengthened. Efficient learning also requires, however, that the synaptic strength be decreased every now and then [[#References|[a2]]]. | ||
− | In the present context, one usually wants to store a number of activity patterns in a network with a fairly high connectivity ( | + | In the present context, one usually wants to store a number of activity patterns in a network with a fairly high connectivity ( $ 10 ^ {4} $ |
+ | in biological nets). Most of the information presented to a network varies in space and time. So what is needed is a common representation of both the spatial and the temporal aspects. As a pattern changes, the system should be able to measure and store this change. How can it do that? | ||
− | For unbiased random patterns in a network with synchronous updating this can be done as follows. The neuronal dynamics in its simplest form is supposed to be given by | + | For unbiased random patterns in a network with synchronous updating this can be done as follows. The neuronal dynamics in its simplest form is supposed to be given by $ S _ {i} ( t + \Delta t ) = { \mathop{\rm sign} } ( h _ {i} ( t ) ) $, |
+ | where $ h _ {i} ( t ) = \sum _ {j} J _ {ij } S _ {j} ( t ) $. | ||
+ | Let $ J _ {ij } $ | ||
+ | be the synaptic strength before the learning session, whose duration is denoted by $ T $. | ||
+ | After the learning session, $ J _ {ij } $ | ||
+ | is to be changed into $ J _ {ij } + \Delta J _ {ij } $ | ||
+ | with | ||
− | + | $$ | |
+ | \Delta J _ {ij } = \epsilon _ {ij } { | ||
+ | \frac{1}{T} | ||
+ | } \sum _ { 0 } ^ { T } S _ {i} ( t + \Delta t ) S _ {j} ( t - \tau _ {ij } ) | ||
+ | $$ | ||
− | (cf. [[#References|[a3]]], [[#References|[a4]]]). The above equation provides a local encoding of the data at the synapse | + | (cf. [[#References|[a3]]], [[#References|[a4]]]). The above equation provides a local encoding of the data at the synapse $ j \rightarrow i $. |
+ | The $ \epsilon _ {ij } $ | ||
+ | is a constant known factor. The learning session having a duration $ T $, | ||
+ | the multiplier $ T ^ {- 1 } $ | ||
+ | in front of the sum takes saturation into account. The neuronal activity $ S _ {i} ( t ) $ | ||
+ | equals $ 1 $ | ||
+ | if neuron $ i $ | ||
+ | is active at time $ t $ | ||
+ | and $ - 1 $ | ||
+ | if it is not. At time $ t + \Delta t $ | ||
+ | it is combined with the signal that arrives at $ i $ | ||
+ | at time $ t $, | ||
+ | i.e., $ S _ {j} ( t - \tau _ {ij } ) $, | ||
+ | where $ \tau _ {ij } $ | ||
+ | is the axonal delay. Here, $ \{ {S _ {i} ( t ) } : {1 \leq i \leq N } \} $, | ||
+ | denotes the pattern as it is taught to the network of size $ N $ | ||
+ | during the learning session of duration $ 0 \leq t \leq T $. | ||
+ | The time unit is $ \Delta t = 1 $ | ||
+ | milliseconds. In the case of asynchronous dynamics, where each time a single neuron is updated randomly, one has to rescale $ \Delta t \pto {1 / N } $ | ||
+ | and the above sum is reduced to an integral as $ N \rightarrow \infty $. | ||
+ | In passing one notes that for constant, spatial, patterns one recovers the Hopfield model [[#References|[a5]]]. | ||
− | Suppose now that the activity | + | Suppose now that the activity $ a $ |
+ | in the network is low, as is usually the case in biological nets, i.e., $ a \approx - 1 $. | ||
+ | Then the appropriate modification of the above learning rule reads | ||
− | + | $$ | |
+ | \Delta J _ {ij } = \epsilon _ {ij } { | ||
+ | \frac{1}{T} | ||
+ | } \sum _ { 0 } ^ { T } S _ {i} ( t + \Delta t ) [ S _ {j} ( t - \tau _ {ij } ) - \mathbf a ] | ||
+ | $$ | ||
− | (cf. [[#References|[a4]]]). Since | + | (cf. [[#References|[a4]]]). Since $ S _ {j} - a \approx 0 $ |
+ | when the presynaptic neuron is not active, one sees that the pre-synaptic neuron is gating. One gets a depression (LTD) if the post-synaptic neuron is inactive and a potentiation (LTP) if it is active. So it is advantageous to have a time window [[#References|[a6]]]: The pre-synaptic neuron should fire slightly before the post-synaptic one. The above Hebbian learning rule can also be adapted so as to be fully integrated in biological contexts [[#References|[a6]]]. The biology of Hebbian learning has meanwhile been confirmed. See the review [[#References|[a7]]]. | ||
− | G. Palm [[#References|[a8]]] has advocated an extremely low activity for efficient storage of stationary data. Out of | + | G. Palm [[#References|[a8]]] has advocated an extremely low activity for efficient storage of stationary data. Out of $ N $ |
+ | neurons, only $ { \mathop{\rm ln} } N $ | ||
+ | should be active. This seems to be advantageous for hardware realizations. | ||
− | In summary, Hebbian learning is efficient since it is local, and it is a powerful algorithm to store spatial or spatio-temporal patterns. If so, why is it that good? As to the why, the succinct answer [[#References|[a3]]] is that synaptic representations are selected according to their resonance with the input data; the stronger the resonance, the larger | + | In summary, Hebbian learning is efficient since it is local, and it is a powerful algorithm to store spatial or spatio-temporal patterns. If so, why is it that good? As to the why, the succinct answer [[#References|[a3]]] is that synaptic representations are selected according to their resonance with the input data; the stronger the resonance, the larger $ \Delta J _ {ij } $. |
+ | In other words, the algorithm "picks" and strengthens only those synapses that match the input pattern. | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[a1]</TD> <TD valign="top"> D.O. Hebb, "The organization of behavior--A neurophysiological theory" , Wiley (1949)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> T.J. Sejnowski, "Statistical constraints on synaptic plasticity" ''J. Theor. Biol'' , '''69''' (1977) pp. 385–389</TD></TR><TR><TD valign="top">[a3]</TD> <TD valign="top"> A.V.M. Herz, B. Sulzer, R. Kühn, J.L. van Hemmen, "The Hebb rule: Storing static and dynamic objects in an associative neural network" ''Europhys. Lett.'' , '''7''' (1988) pp. 663–669 (Hebbian learning reconsidered: Representation of static and dynamic objects in associative neural nets, Biol. Cybern. 60 (1989), 457–467)</TD></TR><TR><TD valign="top">[a4]</TD> <TD valign="top"> J.L. van Hemmen, W. Gerstner, A.V.M. Herz, R. Kühn, M. Vaas, "Encoding and decoding of patterns which are correlated in space and time" G. Dorffner (ed.) , ''Konnektionismus in artificial Intelligence und Kognitionsforschung'' , Springer (1990) pp. 153–162</TD></TR><TR><TD valign="top">[a5]</TD> <TD valign="top"> J.J. Hopfield, "Neural networks and physical systems with emergent collective computational abilities" ''Proc. Nat. Acad. Sci. USA'' , '''79''' (1982) pp. 2554–2558</TD></TR><TR><TD valign="top">[a6]</TD> <TD valign="top"> W. Gerstner, R. Ritz, J.L. van Hemmen, "Why spikes? Hebbian learning and retrieval of time-resolved excitation patterns" ''Biol. Cybern.'' , '''69''' (1993) pp. 503–515 (See also: W. Gerstner and R. Kempter and J.L. van Hemmen and H. Wagner: A neuronal learning rule for sub-millisecond temporal coding, Nature 383 (1996), 76–78)</TD></TR><TR><TD valign="top">[a7]</TD> <TD valign="top"> T.H. Brown, S. Chattarji, "Hebbian synaptic plasticity: Evolution of the contemporary concept" E. Domany (ed.) J.L. van Hemmen (ed.) K. Schulten (ed.) , ''Models of neural networks'' , '''II''' , Springer (1994) pp. 287–314</TD></TR><TR><TD valign="top">[a8]</TD> <TD valign="top"> G. Palm, "Neural assemblies: An alternative approach to artificial intelligence" , Springer (1982)</TD></TR></table> | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> D.O. Hebb, "The organization of behavior--A neurophysiological theory" , Wiley (1949)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> T.J. Sejnowski, "Statistical constraints on synaptic plasticity" ''J. Theor. Biol'' , '''69''' (1977) pp. 385–389</TD></TR><TR><TD valign="top">[a3]</TD> <TD valign="top"> A.V.M. Herz, B. Sulzer, R. Kühn, J.L. van Hemmen, "The Hebb rule: Storing static and dynamic objects in an associative neural network" ''Europhys. Lett.'' , '''7''' (1988) pp. 663–669 (Hebbian learning reconsidered: Representation of static and dynamic objects in associative neural nets, Biol. Cybern. 60 (1989), 457–467)</TD></TR><TR><TD valign="top">[a4]</TD> <TD valign="top"> J.L. van Hemmen, W. Gerstner, A.V.M. Herz, R. Kühn, M. Vaas, "Encoding and decoding of patterns which are correlated in space and time" G. Dorffner (ed.) , ''Konnektionismus in artificial Intelligence und Kognitionsforschung'' , Springer (1990) pp. 153–162</TD></TR><TR><TD valign="top">[a5]</TD> <TD valign="top"> J.J. Hopfield, "Neural networks and physical systems with emergent collective computational abilities" ''Proc. Nat. Acad. Sci. USA'' , '''79''' (1982) pp. 2554–2558</TD></TR><TR><TD valign="top">[a6]</TD> <TD valign="top"> W. Gerstner, R. Ritz, J.L. van Hemmen, "Why spikes? Hebbian learning and retrieval of time-resolved excitation patterns" ''Biol. Cybern.'' , '''69''' (1993) pp. 503–515 (See also: W. Gerstner and R. Kempter and J.L. van Hemmen and H. Wagner: A neuronal learning rule for sub-millisecond temporal coding, Nature 383 (1996), 76–78)</TD></TR><TR><TD valign="top">[a7]</TD> <TD valign="top"> T.H. Brown, S. Chattarji, "Hebbian synaptic plasticity: Evolution of the contemporary concept" E. Domany (ed.) J.L. van Hemmen (ed.) K. Schulten (ed.) , ''Models of neural networks'' , '''II''' , Springer (1994) pp. 287–314</TD></TR><TR><TD valign="top">[a8]</TD> <TD valign="top"> G. Palm, "Neural assemblies: An alternative approach to artificial intelligence" , Springer (1982)</TD></TR></table> |
Latest revision as of 22:10, 5 June 2020
Hebbian learning
A learning rule dating back to D.O. Hebb's classic [a1], which appeared in 1949. The idea behind it is simple. Neurons of vertebrates consist of three parts: a dendritic tree, which collects the input, a soma, which can be considered as a central processing unit, and an axon, which transmits the output. Neurons communicate via action potentials or spikes, pulses of a duration of about one millisecond. If neuron $ j $ emits a spike, it travels along the axon to a so-called synapse on the dendritic tree of neuron $ i $, say. This takes $ \tau _ {ij } $ milliseconds. The synapse has a synaptic strength, to be denoted by $ J _ {ij } $. Its value, which encodes the information to be stored, is to be governed by the Hebb rule.
In [a1], p. 62, one can find the "neurophysiological postulate" that is the Hebb rule in its original form: When an axon of cell $ A $ is near enough to excite a cell $ B $ and repeatedly or persistently takes part in firing it, some growth process or metabolic change takes place in one or both cells such that the efficiency of $ A $, as one of the cells firing $ B $, is increased.
Hebb's postulate has been formulated in plain English (but not more than that) and the main question is how to implement it mathematically. The key ideas are that:
i) only the pre- and post-synaptic neuron determine the change of a synapse;
ii) learning means evaluating correlations. If both $ A $ and $ B $ are active, then the synaptic efficacy should be strengthened. Efficient learning also requires, however, that the synaptic strength be decreased every now and then [a2].
In the present context, one usually wants to store a number of activity patterns in a network with a fairly high connectivity ( $ 10 ^ {4} $ in biological nets). Most of the information presented to a network varies in space and time. So what is needed is a common representation of both the spatial and the temporal aspects. As a pattern changes, the system should be able to measure and store this change. How can it do that?
For unbiased random patterns in a network with synchronous updating this can be done as follows. The neuronal dynamics in its simplest form is supposed to be given by $ S _ {i} ( t + \Delta t ) = { \mathop{\rm sign} } ( h _ {i} ( t ) ) $, where $ h _ {i} ( t ) = \sum _ {j} J _ {ij } S _ {j} ( t ) $. Let $ J _ {ij } $ be the synaptic strength before the learning session, whose duration is denoted by $ T $. After the learning session, $ J _ {ij } $ is to be changed into $ J _ {ij } + \Delta J _ {ij } $ with
$$ \Delta J _ {ij } = \epsilon _ {ij } { \frac{1}{T} } \sum _ { 0 } ^ { T } S _ {i} ( t + \Delta t ) S _ {j} ( t - \tau _ {ij } ) $$
(cf. [a3], [a4]). The above equation provides a local encoding of the data at the synapse $ j \rightarrow i $. The $ \epsilon _ {ij } $ is a constant known factor. The learning session having a duration $ T $, the multiplier $ T ^ {- 1 } $ in front of the sum takes saturation into account. The neuronal activity $ S _ {i} ( t ) $ equals $ 1 $ if neuron $ i $ is active at time $ t $ and $ - 1 $ if it is not. At time $ t + \Delta t $ it is combined with the signal that arrives at $ i $ at time $ t $, i.e., $ S _ {j} ( t - \tau _ {ij } ) $, where $ \tau _ {ij } $ is the axonal delay. Here, $ \{ {S _ {i} ( t ) } : {1 \leq i \leq N } \} $, denotes the pattern as it is taught to the network of size $ N $ during the learning session of duration $ 0 \leq t \leq T $. The time unit is $ \Delta t = 1 $ milliseconds. In the case of asynchronous dynamics, where each time a single neuron is updated randomly, one has to rescale $ \Delta t \pto {1 / N } $ and the above sum is reduced to an integral as $ N \rightarrow \infty $. In passing one notes that for constant, spatial, patterns one recovers the Hopfield model [a5].
Suppose now that the activity $ a $ in the network is low, as is usually the case in biological nets, i.e., $ a \approx - 1 $. Then the appropriate modification of the above learning rule reads
$$ \Delta J _ {ij } = \epsilon _ {ij } { \frac{1}{T} } \sum _ { 0 } ^ { T } S _ {i} ( t + \Delta t ) [ S _ {j} ( t - \tau _ {ij } ) - \mathbf a ] $$
(cf. [a4]). Since $ S _ {j} - a \approx 0 $ when the presynaptic neuron is not active, one sees that the pre-synaptic neuron is gating. One gets a depression (LTD) if the post-synaptic neuron is inactive and a potentiation (LTP) if it is active. So it is advantageous to have a time window [a6]: The pre-synaptic neuron should fire slightly before the post-synaptic one. The above Hebbian learning rule can also be adapted so as to be fully integrated in biological contexts [a6]. The biology of Hebbian learning has meanwhile been confirmed. See the review [a7].
G. Palm [a8] has advocated an extremely low activity for efficient storage of stationary data. Out of $ N $ neurons, only $ { \mathop{\rm ln} } N $ should be active. This seems to be advantageous for hardware realizations.
In summary, Hebbian learning is efficient since it is local, and it is a powerful algorithm to store spatial or spatio-temporal patterns. If so, why is it that good? As to the why, the succinct answer [a3] is that synaptic representations are selected according to their resonance with the input data; the stronger the resonance, the larger $ \Delta J _ {ij } $. In other words, the algorithm "picks" and strengthens only those synapses that match the input pattern.
References
[a1] | D.O. Hebb, "The organization of behavior--A neurophysiological theory" , Wiley (1949) |
[a2] | T.J. Sejnowski, "Statistical constraints on synaptic plasticity" J. Theor. Biol , 69 (1977) pp. 385–389 |
[a3] | A.V.M. Herz, B. Sulzer, R. Kühn, J.L. van Hemmen, "The Hebb rule: Storing static and dynamic objects in an associative neural network" Europhys. Lett. , 7 (1988) pp. 663–669 (Hebbian learning reconsidered: Representation of static and dynamic objects in associative neural nets, Biol. Cybern. 60 (1989), 457–467) |
[a4] | J.L. van Hemmen, W. Gerstner, A.V.M. Herz, R. Kühn, M. Vaas, "Encoding and decoding of patterns which are correlated in space and time" G. Dorffner (ed.) , Konnektionismus in artificial Intelligence und Kognitionsforschung , Springer (1990) pp. 153–162 |
[a5] | J.J. Hopfield, "Neural networks and physical systems with emergent collective computational abilities" Proc. Nat. Acad. Sci. USA , 79 (1982) pp. 2554–2558 |
[a6] | W. Gerstner, R. Ritz, J.L. van Hemmen, "Why spikes? Hebbian learning and retrieval of time-resolved excitation patterns" Biol. Cybern. , 69 (1993) pp. 503–515 (See also: W. Gerstner and R. Kempter and J.L. van Hemmen and H. Wagner: A neuronal learning rule for sub-millisecond temporal coding, Nature 383 (1996), 76–78) |
[a7] | T.H. Brown, S. Chattarji, "Hebbian synaptic plasticity: Evolution of the contemporary concept" E. Domany (ed.) J.L. van Hemmen (ed.) K. Schulten (ed.) , Models of neural networks , II , Springer (1994) pp. 287–314 |
[a8] | G. Palm, "Neural assemblies: An alternative approach to artificial intelligence" , Springer (1982) |
Hebb rule. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Hebb_rule&oldid=16900