Landscape




$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =





Chosen Fixed Point

Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.

#TheorySuperpotentialCentral charge $a$Central charge $c$Ratio $a/c$Matter field: $R$-chargeU(1) part of $F_{UV}$Rank of $F_{UV}$Rational
1802 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{1}^{2}$ 0.6991 0.86 0.8129 [M:[0.7009, 1.1495, 1.0, 0.7009, 1.0], q:[0.7874, 0.5117], qb:[0.5117, 0.4883], phi:[0.4252]] [M:[[1, 15], [0, -4], [-1, -7], [-1, 1], [1, 7]], q:[[0, -1], [-1, -14]], qb:[[1, 0], [0, 7]], phi:[[0, 2]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{4}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{4}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{3}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{2}$ ${}M_{3}^{2}$, ${ }M_{5}^{2}$ -2 2*t^2.103 + 2*t^3. + t^3.07 + t^3.449 + t^3.827 + 4*t^4.206 + 2*t^4.276 + 3*t^4.346 + 4*t^5.103 + 2*t^5.173 + 2*t^5.551 - 2*t^6. + t^6.14 + 6*t^6.308 + 3*t^6.378 + 6*t^6.449 + t^6.519 + 6*t^7.206 + 4*t^7.276 + 4*t^7.346 + 3*t^7.416 + 4*t^7.654 - 4*t^8.103 - t^8.173 + 9*t^8.411 + 6*t^8.481 + 11*t^8.551 + 4*t^8.622 + 5*t^8.692 - t^8.93 - t^4.276/y - (2*t^6.378)/y + t^7.206/y + (4*t^8.103)/y + (4*t^8.173)/y - (3*t^8.481)/y + (2*t^8.551)/y + (2*t^8.93)/y - t^4.276*y - 2*t^6.378*y + t^7.206*y + 4*t^8.103*y + 4*t^8.173*y - 3*t^8.481*y + 2*t^8.551*y + 2*t^8.93*y (g2*t^2.103)/g1 + g1*g2^15*t^2.103 + t^3./(g1*g2^7) + g1*g2^7*t^3. + t^3.07/g2^14 + t^3.449/g2^4 + g2^6*t^3.827 + (g2^2*t^4.206)/g1^2 + 2*g2^16*t^4.206 + g1^2*g2^30*t^4.206 + t^4.276/(g1*g2^5) + g1*g2^9*t^4.276 + t^4.346/(g1^2*g2^26) + t^4.346/g2^12 + g1^2*g2^2*t^4.346 + t^5.103/(g1^2*g2^6) + 2*g2^8*t^5.103 + g1^2*g2^22*t^5.103 + t^5.173/(g1*g2^13) + g1*g2*t^5.173 + t^5.551/(g1*g2^3) + g1*g2^11*t^5.551 - 2*t^6. + t^6.14/g2^28 + (g2^3*t^6.308)/g1^3 + (2*g2^17*t^6.308)/g1 + 2*g1*g2^31*t^6.308 + g1^3*g2^45*t^6.308 + t^6.378/(g1^2*g2^4) + g2^10*t^6.378 + g1^2*g2^24*t^6.378 + t^6.449/(g1^3*g2^25) + (2*t^6.449)/(g1*g2^11) + 2*g1*g2^3*t^6.449 + g1^3*g2^17*t^6.449 + t^6.519/g2^18 + t^7.206/(g1^3*g2^5) + (2*g2^9*t^7.206)/g1 + 2*g1*g2^23*t^7.206 + g1^3*g2^37*t^7.206 + t^7.276/(g1^2*g2^12) + 2*g2^2*t^7.276 + g1^2*g2^16*t^7.276 + t^7.346/(g1^3*g2^33) + t^7.346/(g1*g2^19) + (g1*t^7.346)/g2^5 + g1^3*g2^9*t^7.346 + t^7.416/(g1^2*g2^40) + t^7.416/g2^26 + (g1^2*t^7.416)/g2^12 + t^7.654/(g1^2*g2^2) + 2*g2^12*t^7.654 + g1^2*g2^26*t^7.654 - (2*g2*t^8.103)/g1 - 2*g1*g2^15*t^8.103 - t^8.173/g2^6 + (g2^4*t^8.411)/g1^4 + (2*g2^18*t^8.411)/g1^2 + 3*g2^32*t^8.411 + 2*g1^2*g2^46*t^8.411 + g1^4*g2^60*t^8.411 + t^8.481/(g1^3*g2^3) + (2*g2^11*t^8.481)/g1 + 2*g1*g2^25*t^8.481 + g1^3*g2^39*t^8.481 + t^8.551/(g1^4*g2^24) + (3*t^8.551)/(g1^2*g2^10) + 3*g2^4*t^8.551 + 3*g1^2*g2^18*t^8.551 + g1^4*g2^32*t^8.551 + t^8.622/(g1^3*g2^31) + t^8.622/(g1*g2^17) + (g1*t^8.622)/g2^3 + g1^3*g2^11*t^8.622 + t^8.692/(g1^4*g2^52) + t^8.692/(g1^2*g2^38) + t^8.692/g2^24 + (g1^2*t^8.692)/g2^10 + g1^4*g2^4*t^8.692 - g2^14*t^8.93 - (g2^2*t^4.276)/y - (g2^3*t^6.378)/(g1*y) - (g1*g2^17*t^6.378)/y + (g2^16*t^7.206)/y + t^8.103/(g1^2*g2^6*y) + (2*g2^8*t^8.103)/y + (g1^2*g2^22*t^8.103)/y + (2*t^8.173)/(g1*g2^13*y) + (2*g1*g2*t^8.173)/y - (g2^4*t^8.481)/(g1^2*y) - (g2^18*t^8.481)/y - (g1^2*g2^32*t^8.481)/y + t^8.551/(g1*g2^3*y) + (g1*g2^11*t^8.551)/y + (g2^7*t^8.93)/(g1*y) + (g1*g2^21*t^8.93)/y - g2^2*t^4.276*y - (g2^3*t^6.378*y)/g1 - g1*g2^17*t^6.378*y + g2^16*t^7.206*y + (t^8.103*y)/(g1^2*g2^6) + 2*g2^8*t^8.103*y + g1^2*g2^22*t^8.103*y + (2*t^8.173*y)/(g1*g2^13) + 2*g1*g2*t^8.173*y - (g2^4*t^8.481*y)/g1^2 - g2^18*t^8.481*y - g1^2*g2^32*t^8.481*y + (t^8.551*y)/(g1*g2^3) + g1*g2^11*t^8.551*y + (g2^7*t^8.93*y)/g1 + g1*g2^21*t^8.93*y


Deformation

Here is the data for the deformed fixed points from the chosen fixed point.

#SuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


Equivalent Fixed Points from Other Seed Theories

Here is a list of equivalent fixed points from other gauge theories.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


Equivalent Fixed Points from the Same Seed Theory

Below is a list of equivalent fixed points from the same seed theories.

id Theory Superpotential Central Charge $a$ Central Charge $c$ Ratio $a/c$ $R$-charges More Info. Rational


Previous Theory

The previous fixed point before deforming to get the chosen fixed point.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
338 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{5}$ 0.7184 0.8775 0.8187 [M:[0.8179, 1.091, 1.0, 0.8179, 1.0], q:[0.6411, 0.541], qb:[0.541, 0.459], phi:[0.4545]] 2*t^2.454 + 2*t^3. + t^3.246 + t^3.273 + t^3.3 + t^4.118 + 2*t^4.363 + 3*t^4.609 + t^4.664 + 3*t^4.907 + 2*t^4.91 + t^5.21 + 3*t^5.454 + 2*t^5.727 - 3*t^6. - t^4.363/y - t^4.363*y detail