The boundary seam algebras b n,k (β = q + q −1 ) were introduced by Morin-Duchesne, Ridout and Rasmussen to formulate algebraically a large class of boundary conditions for two-dimensional statistical loop models. The representation theory of these algebras b n,k (β = q + q −1 ) is given: their irreducible, standard (cellular) and principal modules are constructed and their structure explicited in terms of their composition factors and of non-split short exact sequences. The dimensions of the irreducible modules and of the radicals of standard ones are also given. The methods proposed here might be applicable to a large family of algebras, for example to those introduced recently by Flores and Peltola, and Crampé and Poulain d'Andecy.The boundary seam algebras, or seam algebras for short, were introduced by Morin-Duchesne, Ridout and Rasmussen [1]. One of their goals was to cast, in an algebraic setting, various boundary conditions of two-dimensional statistical loop models discovered earlier in a heuristic way (see for example [2]). Not only did the authors define diagrammatically the seam algebras, give them a presentation through generators and relations and prove equivalence between the definitions, but they also introduced standard modules over b n,k and computed the Gram determinant of an invariant bilinear Date: November 28, 2019. Key words and phrases. Temperley-Lieb algebra, Temperley-Lieb seam algebra, boundary seam algebra, seam algebra, cellular algebra, cellular module, standard module, projective module, principal indecomposable module, non-semisimple associative algebras. 1 REPRESENTATION THEORY OF SEAM ALGEBRAS 2 form on these modules. All these tools will be used here. Their paper went on with numerical computation of the spectra of the loop transfer matrices under these various boundary conditions. It indicated a potentially rich representation theory.In its simplest formulation, the seam algebra b n,k is the subset of the Temperley-Lieb algebra TL n+k (β ) [3] obtained by left-and right-multiplying all its elements by a Wenzl-Jones projector [4,5] acting on k of the n + k points. Even though this formulation appears first in [1], the need for some algebraic structure of this type was stressed before by Jacobsen and Saleur [6]. The main goal of their paper was also the study of various boundary conditions for loop models. In a short section at the end of their paper, these authors observed that the blob algebra (see below) can be realized by adding "ghost" strings to link diagrams (their cabling construction) and "tying" them with the first "real" string with a projector. But their goal did not require a formal definition of a new algebra. The definition of the seam algebra b n,k will be given in section 2 and it will be seen there that it is actually a quotient of the blob algebra. So the seam algebras are yet another variation of the original Temperley-Lieb family. The representation theory of various Temperley-Lieb families has been studied, displaying remarkable richness and diversity: the b...