Cognitive Theorist Paper
University of Phoenix
Jeffery Butler
PSY/390
December 03, 2015
Cognitive Theorist Paper
Edward C. Tolman contributed substantially to the research of learning and motivation to
the field of psychology. He acquired his specific beh
Introduction to Learning Paper
University of Phoenix
Jeffery Butler
PSY/390
November 13, 2015
Introduction to Learning Paper
Learning is defined by the acquisition of knowledge. It can be described as a comparison
continuing change in conduct that is the
Week One: Introduction to Learning and Cognition
Details
Due
Objectives
1.1 Define learning and its behavioral component.
1.2 Describe different types of learning.
1.3 Analyze the relationship between learning and
cognition.
1.4 Apply learning and cogniti
Functionalism: B.F. Skinner
and
Associationistic: Ivan Pavlov
Ella Bokman, Dominique Gebhard, Alice
Stonick, and Darla Fisher
Psy/390
May 14, 2012
Kay Rubin
Functionalism and Associationistic
Theories
Functionalism examines the active
psychological proces
FUNCTIONALISTIC AND
ASSOCIATIONISTIC
THEORIES PRESENTATION
BY: TEAM B (CESAR LARIOS, SARA UNDERWOOD, SHANAE DUNN
TABLE OF CONTENTS
Introduction
Ivan Pavlov Bio
B. F. Skinner Bio
Associationistic Theories
Functionalistic Theories
Contributions made t
Running head: INDIVIDUAL PROGRAMMATIC ASSESSMENT
Individual Programmatic Assessment
Cesar Larios
PSY 390
February 5, 2016
Jennifer MacLure
1
INDIVIDUAL PROGRAMMATIC ASSESSMENT
2
Individual Programmatic Assessment
Learning is an activity that most of perfo
Running head: INTRODUCTION TO LEARNING PAPER
Introduction to Learning Paper
Cesar Larios
PSY 390
August 24, 2015
Bruce Thiessen
1
INTRODUCTION TO LEARNING PAPER
2
Introduction to Learning Paper
Learning is one of the most important task that we perform as
Cognitive Theories
Focus on the Thought Processes and Sensory Input methods
Established by Albert Bandura
Neuro-Physiological Theories
Focus on the actual physiological methods that
occurs in the brain as a human being is taught
Established by Donald Hebb
FUNCTIONALISTIC
AND
ASSOCIATIONISTIC
THEORIES
PSY390
INTRODUCTION
Different theories of behavior are presented by
both B. F. Skinner and Ivan Pavlov. Skinners is
known as operant conditioning while Pavlovs
theory is known as classical conditioning. While
Running head: OPERANT CONDITIONING
Operant Conditioning
PSY/390
May 5, 2014
Gary Burk
1
OPERANT CONDITIONING
2
Operant Conditioning
Introduction
There have been many theories introduced into psychology over the past century and one
of the most popular and
Operant Conditioning Paper 1
CERTIFICATE OF ORIGINALITY: I certify that the attached paper is my original work. I affirm that any
section of the paper which has been submitted previously is attributed and cited as such, and that this
paper has not been su
Running head: LEARNING AND COGNITION PAPER
Learning and Cognition Paper
PSY/390
April 28, 2014
Gary Burk
1
LEARNING AND COGNITION PAPER
2
Learning and Cognition Paper
Introduction
From birth the process of learning begins and continues until our death. Le
Running head: LEARNING AND COGNITION
1
Learning and Cognition
Introduction
I think therefore I am (Skirry, 2008). If it can be imagine, comprehend and processed,
then it can be learned. Through sensory perception, in the environment, through individual
in
Running head: LEARNING AND COGNITION
1
Learning and Cognition
Introduction
I think therefore I am (Skirry, 2008). If it can be imagine, comprehend and processed,
then it can be learned. Through sensory perception, in the environment, through individual
in
Running head: LEARNING AND COGNITION PAPER
Learning and Cognition Paper
Kristopher Knutson
PSY/390
April 28, 2014
Gary Burk
1
LEARNING AND COGNITION PAPER
2
Learning and Cognition Paper
Introduction
From birth the process of learning begins and continues
Running head: OPERANT CONDITIONING
Chagoll Brown
Operant Conditioning
Professor Esther Siler Colbert
PSY/390
1
OPERANT CONDITIONING
2
Operant Conditioning
B. F. Skinner is viewed as the father of Operant Conditioning he trusted that the most ideal
approac
B ERTFRIE D FAUSER U NIVERSIT Y
OF
117
KONSTANZ
where we have used the following abbreviations
I := cfw_, , rK := cfw_k, , zP tr := 1 1
DI
I
1 2
I 1 I2
U
I 2 I 3 I4
I1
L
:= (i0 k k 0 m)
:= e0 (0
:=
e02
2
(r1 r2 )
1
2
1 2
2
(C 0)
2
3
2
1
4
2
2 3
(r2 r3)(
160
A Treatise on Quantum Clifford Algebras
[40] Albert Crumeyrolle. Orthogonal and Symplectic Clifford Algebra Spinor Structures.
Kluwer Academic Publishers, Dordrecht, 1990.
[41] John de Pills. Grassmann algebras as Hilbert space. Journal of Algebra, 10
116
8.1
A Treatise on Quantum Clifford Algebras
Field equations
To be able to define a QFT we need two informations: (i) a field equation and (ii) (anti)commutation rules. The Lagrangian point of view is more sophisticated and mostly chosen to incorporate
Chapter 8
(Fermionic) quantum fi eld theory and
Clifford Hopf gebra
In this chapter we develop a formulation of fermionic quantum field theory (QFT) based on Hopf
gebraic methods. We concentrate on fermions, however, the bosonic case runs along the same
l
114
A Treatise on Quantum Clifford Algebras
product &r with a renormalized time-ordered operator product and the coefficients derived therefrom, see Brouders paper. The cliffordization results in a tremendous simple formula for the
renormalized Green func
B ERTFRIE D FAUSER U NIVERSIT Y
OF
KONSTANZ
113
difficult for a long time. Both such structures are quantized due to the introduction of a symmetric
bilinear form g extended by exponentiation to g in the same manner.
Brouder imposed on the Z -mappings the
B ERTFRIE D FAUSER U NIVERSIT Y
OF
KONSTANZ
holds. If the above discussed maps A and B are Z2 -graded, we find for the prefactor
|x |x |+|A(x(2) )|B (x(1)|
2|x |x |
(1) (1) (2)
= () (1) (2) = +1
and the corresponding convolution product is commutative, he
112
A Treatise on Quantum Clifford Algebras
can be identified with the time-ordered products the dotted wedge corresponds to the normalordered case. In our previously published works, we had restricted this mechanism to Hamilton
formalism, which relays on
110
A Treatise on Quantum Clifford Algebras
We assume that the convolution is w.r.t. a Gramann Hopf gebra or a symmetric such Hopf gebra,
which might be called Weyl Hopf gebra. In this case it is possible to deduce the convolutive unit
to be u = . Such Ho
B ERTFRIE D FAUSER U NIVERSIT Y
OF
KONSTANZ
and
BF
If we write this in algebraic terms using Sweedler notation, we obtain for arbitrary elements
V
u, v, w V
BF(u v, w) = BF(u, w )BF(v, w )
and
(2)
(1)
BF(u, v w) = BF(u(1), w)BF(u(2), v).
(7-33)
This is in
108
A Treatise on Quantum Clifford Algebras
Therefore, since we want to go for renormalization, one has to assert that (anti)commutation relations are not altered by the generalized cliffordization process and thus by the renormalization
process. But, thi
106
A Treatise on Quantum Clifford Algebras
with an arbitrary bilinear form BF, &r may not even be unital. We need further more that the
co-product is an algebra homomorphism
(a b) = (a b)(1) (a b)(2)
= (1)|a(2) |b(1) | (a b ) (a
(1)
(1)
b ).
(2)
(7-16)
(
B ERTFRIE D FAUSER U NIVERSIT Y
OF
KONSTANZ
107
This yields
(1)|u(1) | BF(u(2), v(1) BF(u(1), w(2) BF(v(2), w(1) =
(1)|w(2) | BF(u, v(1) w(2) BF(v(2), w(1).
(7-23)
Cancelling out the common factor and renaming yield the product co-product duality up to a
B ERTFRIE D FAUSER U NIVERSIT Y
OF
105
KONSTANZ
Let GB = cfw_Id, e1 , . . . , en , e1 e2 , . . . be a canonical Gramann basis of
X = X0 Id +
X
Xi ei +
i
X
V
V . An element
Xij ei ej + . . . X1.n e1 . . . en
(7-12)
i<j
where some or all Xir ,. ,is are non-